Home |
Search |
Today's Posts |
#11
![]() |
|||
|
|||
![]()
Dead-zone = phase noise. Very little dead-zone = very little phase noise.
Bigger dead-zone = bigger phase noise. You can interpolate the rest for yourself. Joe W3JDR "Avery Fineman" wrote in message ... In article B_Htc.4677$pt3.1214@attbi_s03, "Rick Karlquist N6RK" writes: There are various fixes for the dead zone problem. In the mid-1970's, Fairchild (the original company) sold an "11C44" phase detector that got rid of the dead zone by injecting a narrow pulse so that the phase detector pulses would never have to try to go to zero width. Eric Breeze holds the patent on this technique; if interested read his patent. Analog Devices makes that AD9901 phase detector which gets around the dead zone by first dividing the frequency by 2. However, it is not suitable for a frequency synthesizer because of the large spurious sidebands resulting from this technique. Motorola had some patents on the circuits in its MC145159 that dealt with the dead zone and sampling sidebands. It also used a divide by 2 technique, that was not documented; (we figured it out by observing the chip's output). That chip may have been inherited by On Semiconductor. It was originally developed for some division of GE. The "dead zone problem" is less a problem and more a state of mind. :-) When implemented with a charge-pump circuit (voltage & time converter to current) between the PFD and loop filter, it rather disappears into the woodwork of the whole PLL. The phase difference between signal and reference is proportional to the control voltage of the VCO producing the basic frequency. There is ALWAYS going to be a signal versus reference phase offset when the entire loop is in lock so this dreaded "dead zone problem" will only show up in a very narrow range of controlled frequency. General intuitive thought on any PLL or other synthesizer closed loop is that the relative phase between signal and reference is zero. It isn't. If it was, then the VCO could not be controlled. As a very rough indicator of VCO frequency, that signal v. reference offset phase exists for quick scope checking...when the control voltage range of the VCO is known. Good for a quick bench check. In practical terms, that dreaded "dead zone" isn't visible in a real-world example. Case in point: 23+ years ago, Rocketdyne Division of Rockwell International (now a Division of Boeing) was beginning work on a Deformable Mirror for laser work (they had a sizeable optics group) that used a 1 MHz signal out of optics to indicate the light phase error of an optical interferometer. I rigged up a 74H family phase-frequency detector circuit as the heart of that, an integrator out of that into an A-to-D converter to get a digital version for computer data manipulation. By all the careful measurement, the expected dead zone didn't show up on any graphing and the standard lab time interval counters could resolve, accurately, 2 nanoseconds using time averaging. [translates to rather less than a degree of phase error] The optical physicists had been hopping up and down about "dead zone" in meetings but the actual circuit performance didn't show it. One reason for the non-observation of any dead zone is that the digital gates forming the PFD were so lightly loaded in other-gate capacitance that their propagation delays all tended to be the same. Datasheet values of propagation delay of gates are all given as maximums, rather worst-case things with lots of pFds connected to outputs, etc. Put on half a prototype board, loaded only by other gates of the PFD and the resistor input of an op-amp integrator, the capacitance loading was minimal. [project was successful, and spawned more work on deformable mirrors] It can be an interesting academic problem to achieve a zero dead- dead zone effect in a PFD, but thats about it. When working at the comparison frequency of less than a few MHz, the PFD dead zone due to differential propagation delays of the gates disappears into the woodwork when using 74LS or faster digital families. There's plenty to be concerned about in any frequency synthesizer subsystem, but a phase-frequency detector gate structure is a very minor problem in my opinion. DDS and fractional-N loops in synthesizers have their own problems such as spurious output, but those problems can't really be traced to any PFD dead-zone effect. A PFD is wonderful as a control loop element in that it can control a VCO (of the loop) from way off the frequency and bring it into a lock phase range...from either worst- case start-up frequency. [way back in the beginning of radio time, lock loops had to use sawtooth sweep circuits to cure that start-up condition, and couldn't control beyond +/- 90 degrees of phase shift...PFDs easily handle +/-180 degrees] Len Anderson retired (from regular hours) electronic engineer person |
#12
![]() |
|||
|
|||
![]()
In article , "W3JDR"
writes: Dead-zone = phase noise. Very little dead-zone = very little phase noise. Bigger dead-zone = bigger phase noise. You can interpolate the rest for yourself. I have to disagree with some of that. First of all, a "dead zone" or the almost-exactly-in-phase condition, occurs at only one VCO frequency where the control voltage sets up the frequency for that in-phase condition. Yes, at that exact frequency, there COULD be some phase noise. But, the phase noise may NOT be from this "dead zone" effect. Phase noise can come from MANY different sources. If it occurs well away from the in-same-phase "dead zone" then the phase noise is NOT caused by any "dead zone." The relative phase between signal and reference inputs to a PFD correspond to the VCO control voltage (times the charge-pump or integrator circuit constants). Signal and reference phases when in lock will always be offset from one another, one leading and one lagging. A good loop will show a constant offset of phases even when both inputs hold a constant phase. Len Anderson |
#13
![]() |
|||
|
|||
![]()
In article , "W3JDR"
writes: Dead-zone = phase noise. Very little dead-zone = very little phase noise. Bigger dead-zone = bigger phase noise. You can interpolate the rest for yourself. I have to disagree with some of that. First of all, a "dead zone" or the almost-exactly-in-phase condition, occurs at only one VCO frequency where the control voltage sets up the frequency for that in-phase condition. Yes, at that exact frequency, there COULD be some phase noise. But, the phase noise may NOT be from this "dead zone" effect. Phase noise can come from MANY different sources. If it occurs well away from the in-same-phase "dead zone" then the phase noise is NOT caused by any "dead zone." The relative phase between signal and reference inputs to a PFD correspond to the VCO control voltage (times the charge-pump or integrator circuit constants). Signal and reference phases when in lock will always be offset from one another, one leading and one lagging. A good loop will show a constant offset of phases even when both inputs hold a constant phase. Len Anderson |
#14
![]() |
|||
|
|||
![]()
In article , "Steve Nosko"
writes: "Avery Fineman" wrote in message ... In article B_Htc.4677$pt3.1214@attbi_s03, "Rick Karlquist N6RK" writes: There are various fixes for the dead zone problem. In the mid-1970's, Fairchild (the original company) sold an "11C44" phase detector that got rid of the dead zone by injecting a narrow pulse so that the phase detector pulses would never have to try to go to zero width. Eric Breeze holds the patent on this technique; if interested read his patent. Analog Devices makes that AD9901 phase detector which gets around the dead zone by first dividing the frequency by 2. However, it is not suitable for a frequency synthesizer because of the large spurious sidebands resulting from this technique. Motorola had some patents on the circuits in its MC145159 that dealt with the dead zone and sampling sidebands. It also used a divide by 2 technique, that was not documented; (we figured it out by observing the chip's output). That chip may have been inherited by On Semiconductor. It was originally developed for some division of GE. The "dead zone problem" is less a problem and more a state of mind. :-) When implemented with a charge-pump circuit (voltage & time converter to current) between the PFD and loop filter, it rather disappears into the woodwork of the whole PLL. The phase difference between signal and reference is proportional to the control voltage of the VCO producing the basic frequency. There is ALWAYS going to be a signal versus reference phase offset when the entire loop is in lock so this dreaded "dead zone problem" will only show up in a very narrow range of controlled frequency. General intuitive thought on any PLL or other synthesizer closed loop is that the relative phase between signal and reference is zero. It isn't. If it was, then the VCO could not be controlled. As a very rough indicator of VCO frequency, that signal v. reference offset phase exists for quick scope checking...when the control voltage range of the VCO is known. Good for a quick bench check. In practical terms, that dreaded "dead zone" isn't visible in a real-world example. Case in point: 23+ years ago, Rocketdyne Division of Rockwell International (now a Division of Boeing) was beginning work on a Deformable Mirror for laser work (they had a sizeable optics group) that used a 1 MHz signal out of optics to indicate the light phase error of an optical interferometer. I rigged up a 74H family phase-frequency detector circuit as the heart of that, an integrator out of that into an A-to-D converter to get a digital version for computer data manipulation. By all the careful measurement, the expected dead zone didn't show up on any graphing and the standard lab time interval counters could resolve, accurately, 2 nanoseconds using time averaging. [translates to rather less than a degree of phase error] The optical physicists had been hopping up and down about "dead zone" in meetings but the actual circuit performance didn't show it. One reason for the non-observation of any dead zone is that the digital gates forming the PFD were so lightly loaded in other-gate capacitance that their propagation delays all tended to be the same. Datasheet values of propagation delay of gates are all given as maximums, rather worst-case things with lots of pFds connected to outputs, etc. Put on half a prototype board, loaded only by other gates of the PFD and the resistor input of an op-amp integrator, the capacitance loading was minimal. [project was successful, and spawned more work on deformable mirrors] It can be an interesting academic problem to achieve a zero dead- dead zone effect in a PFD, but thats about it. When working at the comparison frequency of less than a few MHz, the PFD dead zone due to differential propagation delays of the gates disappears into the woodwork when using 74LS or faster digital families. There's plenty to be concerned about in any frequency synthesizer subsystem, but a phase-frequency detector gate structure is a very minor problem in my opinion. DDS and fractional-N loops in synthesizers have their own problems such as spurious output, but those problems can't really be traced to any PFD dead-zone effect. A PFD is wonderful as a control loop element in that it can control a VCO (of the loop) from way off the frequency and bring it into a lock phase range...from either worst- case start-up frequency. [way back in the beginning of radio time, lock loops had to use sawtooth sweep circuits to cure that start-up condition, and couldn't control beyond +/- 90 degrees of phase shift...PFDs easily handle +/-180 degrees] Len Anderson retired (from regular hours) electronic engineer person Len - Avery, whomever, Our experiences differ. When designing PLL synths back then for two-war radio, we always saw the dead zone. "Two-war radio?" PRC-25? Term not understood. Experience has hands-on with everything from a PRC-8 to a PRC-104, but little with the PRC-25 or -77. In a type 2 loop (hope I'm remembering my control theory correctly) the extra integration allows the VCO to float around within the dead zone, causing a low freq rumble at times. You could watch the phase wandering around on a scope on the two PD inputs. If the loop is set for something like a 10 to 50 mSec lock-in time, one has to look quick to see the actual lock-in. If the loop is designed properly (VCO control voltage gain, time relative to the reference frequency), there should not be any "wander." In order to see the settling time from a large step-function of frequency change, you need to sync a scope from the step source and watch the jump-and-settle of the control voltage like a damped sinewave. That's a quick check of loop control action. Storage scope (old way) or digital scope (muy better) are the best way to view that. We would force some small leakage current just to hold it up against one side of the dead zone. Perhaps the types of requirements causes the difference. We were in the audio range with the PD reference freq and lock times in the tens of ms. if I recall correctly. Most of the older PLLs had reference frequencies of 1 to 5 KHz. That's a period of 1.0 mS to 200 uS. Without about 5 to 10 cycles for settling-in (to near invisibility), that would be about 10 to 2 mS, rather quick. If I recall, the Fairchild chip did a better job of matching the delays. The small overlap causing a narrow pulse to occur seemed like a small issue - not much energy at the ref freq for some applications. Our synthesizers were of such requirements that there was a very tight balance between lock time and spurious. The loop filtering took much care to get the lock time and keep reference spurs down. Regardless of the loop filter type, those are always fussy to avoid pickup contamination of the VCO control line. But, knowing the control voltage characteristics (delta-V v. frequency) over a range, the design is strictly textbook formula stuff. It helps greatly if the VCO control characteristics are linear versus frequency AND the division ratio maximum to minimum number is as small as possible. I've seen a few applications where both the control voltage characteristics were very non-linear AND the division ratio of the PLL greater than 2:1 with the end result being an almost impossible lock at the extreme ends of the tuning range. One case was alleviated by extra circuitry from the division control to generate a DC bias summed with the control voltage. Not too swift since it took more parts, but better than failure. In my own case, the filtering and shielding around the PFD to VCO had to be rather severe in order to keep it stable (too much high-energy circuitry rather nearby). Once that was achieved, there was no wandering at a 1 KHz reference input with proper values of known control voltage constants and accurate calculation of loop filter values. It was "tight." Len Anderson |
#15
![]() |
|||
|
|||
![]()
In article , "Steve Nosko"
writes: "Avery Fineman" wrote in message ... In article B_Htc.4677$pt3.1214@attbi_s03, "Rick Karlquist N6RK" writes: There are various fixes for the dead zone problem. In the mid-1970's, Fairchild (the original company) sold an "11C44" phase detector that got rid of the dead zone by injecting a narrow pulse so that the phase detector pulses would never have to try to go to zero width. Eric Breeze holds the patent on this technique; if interested read his patent. Analog Devices makes that AD9901 phase detector which gets around the dead zone by first dividing the frequency by 2. However, it is not suitable for a frequency synthesizer because of the large spurious sidebands resulting from this technique. Motorola had some patents on the circuits in its MC145159 that dealt with the dead zone and sampling sidebands. It also used a divide by 2 technique, that was not documented; (we figured it out by observing the chip's output). That chip may have been inherited by On Semiconductor. It was originally developed for some division of GE. The "dead zone problem" is less a problem and more a state of mind. :-) When implemented with a charge-pump circuit (voltage & time converter to current) between the PFD and loop filter, it rather disappears into the woodwork of the whole PLL. The phase difference between signal and reference is proportional to the control voltage of the VCO producing the basic frequency. There is ALWAYS going to be a signal versus reference phase offset when the entire loop is in lock so this dreaded "dead zone problem" will only show up in a very narrow range of controlled frequency. General intuitive thought on any PLL or other synthesizer closed loop is that the relative phase between signal and reference is zero. It isn't. If it was, then the VCO could not be controlled. As a very rough indicator of VCO frequency, that signal v. reference offset phase exists for quick scope checking...when the control voltage range of the VCO is known. Good for a quick bench check. In practical terms, that dreaded "dead zone" isn't visible in a real-world example. Case in point: 23+ years ago, Rocketdyne Division of Rockwell International (now a Division of Boeing) was beginning work on a Deformable Mirror for laser work (they had a sizeable optics group) that used a 1 MHz signal out of optics to indicate the light phase error of an optical interferometer. I rigged up a 74H family phase-frequency detector circuit as the heart of that, an integrator out of that into an A-to-D converter to get a digital version for computer data manipulation. By all the careful measurement, the expected dead zone didn't show up on any graphing and the standard lab time interval counters could resolve, accurately, 2 nanoseconds using time averaging. [translates to rather less than a degree of phase error] The optical physicists had been hopping up and down about "dead zone" in meetings but the actual circuit performance didn't show it. One reason for the non-observation of any dead zone is that the digital gates forming the PFD were so lightly loaded in other-gate capacitance that their propagation delays all tended to be the same. Datasheet values of propagation delay of gates are all given as maximums, rather worst-case things with lots of pFds connected to outputs, etc. Put on half a prototype board, loaded only by other gates of the PFD and the resistor input of an op-amp integrator, the capacitance loading was minimal. [project was successful, and spawned more work on deformable mirrors] It can be an interesting academic problem to achieve a zero dead- dead zone effect in a PFD, but thats about it. When working at the comparison frequency of less than a few MHz, the PFD dead zone due to differential propagation delays of the gates disappears into the woodwork when using 74LS or faster digital families. There's plenty to be concerned about in any frequency synthesizer subsystem, but a phase-frequency detector gate structure is a very minor problem in my opinion. DDS and fractional-N loops in synthesizers have their own problems such as spurious output, but those problems can't really be traced to any PFD dead-zone effect. A PFD is wonderful as a control loop element in that it can control a VCO (of the loop) from way off the frequency and bring it into a lock phase range...from either worst- case start-up frequency. [way back in the beginning of radio time, lock loops had to use sawtooth sweep circuits to cure that start-up condition, and couldn't control beyond +/- 90 degrees of phase shift...PFDs easily handle +/-180 degrees] Len Anderson retired (from regular hours) electronic engineer person Len - Avery, whomever, Our experiences differ. When designing PLL synths back then for two-war radio, we always saw the dead zone. "Two-war radio?" PRC-25? Term not understood. Experience has hands-on with everything from a PRC-8 to a PRC-104, but little with the PRC-25 or -77. In a type 2 loop (hope I'm remembering my control theory correctly) the extra integration allows the VCO to float around within the dead zone, causing a low freq rumble at times. You could watch the phase wandering around on a scope on the two PD inputs. If the loop is set for something like a 10 to 50 mSec lock-in time, one has to look quick to see the actual lock-in. If the loop is designed properly (VCO control voltage gain, time relative to the reference frequency), there should not be any "wander." In order to see the settling time from a large step-function of frequency change, you need to sync a scope from the step source and watch the jump-and-settle of the control voltage like a damped sinewave. That's a quick check of loop control action. Storage scope (old way) or digital scope (muy better) are the best way to view that. We would force some small leakage current just to hold it up against one side of the dead zone. Perhaps the types of requirements causes the difference. We were in the audio range with the PD reference freq and lock times in the tens of ms. if I recall correctly. Most of the older PLLs had reference frequencies of 1 to 5 KHz. That's a period of 1.0 mS to 200 uS. Without about 5 to 10 cycles for settling-in (to near invisibility), that would be about 10 to 2 mS, rather quick. If I recall, the Fairchild chip did a better job of matching the delays. The small overlap causing a narrow pulse to occur seemed like a small issue - not much energy at the ref freq for some applications. Our synthesizers were of such requirements that there was a very tight balance between lock time and spurious. The loop filtering took much care to get the lock time and keep reference spurs down. Regardless of the loop filter type, those are always fussy to avoid pickup contamination of the VCO control line. But, knowing the control voltage characteristics (delta-V v. frequency) over a range, the design is strictly textbook formula stuff. It helps greatly if the VCO control characteristics are linear versus frequency AND the division ratio maximum to minimum number is as small as possible. I've seen a few applications where both the control voltage characteristics were very non-linear AND the division ratio of the PLL greater than 2:1 with the end result being an almost impossible lock at the extreme ends of the tuning range. One case was alleviated by extra circuitry from the division control to generate a DC bias summed with the control voltage. Not too swift since it took more parts, but better than failure. In my own case, the filtering and shielding around the PFD to VCO had to be rather severe in order to keep it stable (too much high-energy circuitry rather nearby). Once that was achieved, there was no wandering at a 1 KHz reference input with proper values of known control voltage constants and accurate calculation of loop filter values. It was "tight." Len Anderson |
#16
![]() |
|||
|
|||
![]()
Everyone please read the 11C44 datasheet at:
http://ira.club.atnet.at/rd/11c44/11C44.html before declaring there is no dead zone. See figure 11. Rick N6RK "Avery Fineman" wrote in message ... In article B_Htc.4677$pt3.1214@attbi_s03, "Rick Karlquist N6RK" writes: There are various fixes for the dead zone problem. In the mid-1970's, Fairchild (the original company) sold an "11C44" phase detector that got rid of the dead zone by injecting a narrow pulse so that the phase detector pulses would never have to try to go to zero width. Eric Breeze holds the patent on this technique; if interested read his patent. Analog Devices makes that AD9901 phase detector which gets around the dead zone by first dividing the frequency by 2. However, it is not suitable for a frequency synthesizer because of the large spurious sidebands resulting from this technique. Motorola had some patents on the circuits in its MC145159 that dealt with the dead zone and sampling sidebands. It also used a divide by 2 technique, that was not documented; (we figured it out by observing the chip's output). That chip may have been inherited by On Semiconductor. It was originally developed for some division of GE. The "dead zone problem" is less a problem and more a state of mind. :-) When implemented with a charge-pump circuit (voltage & time converter to current) between the PFD and loop filter, it rather disappears into the woodwork of the whole PLL. The phase difference between signal and reference is proportional to the control voltage of the VCO producing the basic frequency. There is ALWAYS going to be a signal versus reference phase offset when the entire loop is in lock so this dreaded "dead zone problem" will only show up in a very narrow range of controlled frequency. General intuitive thought on any PLL or other synthesizer closed loop is that the relative phase between signal and reference is zero. It isn't. If it was, then the VCO could not be controlled. As a very rough indicator of VCO frequency, that signal v. reference offset phase exists for quick scope checking...when the control voltage range of the VCO is known. Good for a quick bench check. In practical terms, that dreaded "dead zone" isn't visible in a real-world example. Case in point: 23+ years ago, Rocketdyne Division of Rockwell International (now a Division of Boeing) was beginning work on a Deformable Mirror for laser work (they had a sizeable optics group) that used a 1 MHz signal out of optics to indicate the light phase error of an optical interferometer. I rigged up a 74H family phase-frequency detector circuit as the heart of that, an integrator out of that into an A-to-D converter to get a digital version for computer data manipulation. By all the careful measurement, the expected dead zone didn't show up on any graphing and the standard lab time interval counters could resolve, accurately, 2 nanoseconds using time averaging. [translates to rather less than a degree of phase error] The optical physicists had been hopping up and down about "dead zone" in meetings but the actual circuit performance didn't show it. One reason for the non-observation of any dead zone is that the digital gates forming the PFD were so lightly loaded in other-gate capacitance that their propagation delays all tended to be the same. Datasheet values of propagation delay of gates are all given as maximums, rather worst-case things with lots of pFds connected to outputs, etc. Put on half a prototype board, loaded only by other gates of the PFD and the resistor input of an op-amp integrator, the capacitance loading was minimal. [project was successful, and spawned more work on deformable mirrors] It can be an interesting academic problem to achieve a zero dead- dead zone effect in a PFD, but thats about it. When working at the comparison frequency of less than a few MHz, the PFD dead zone due to differential propagation delays of the gates disappears into the woodwork when using 74LS or faster digital families. There's plenty to be concerned about in any frequency synthesizer subsystem, but a phase-frequency detector gate structure is a very minor problem in my opinion. DDS and fractional-N loops in synthesizers have their own problems such as spurious output, but those problems can't really be traced to any PFD dead-zone effect. A PFD is wonderful as a control loop element in that it can control a VCO (of the loop) from way off the frequency and bring it into a lock phase range...from either worst- case start-up frequency. [way back in the beginning of radio time, lock loops had to use sawtooth sweep circuits to cure that start-up condition, and couldn't control beyond +/- 90 degrees of phase shift...PFDs easily handle +/-180 degrees] Len Anderson retired (from regular hours) electronic engineer person |
#17
![]() |
|||
|
|||
![]()
Everyone please read the 11C44 datasheet at:
http://ira.club.atnet.at/rd/11c44/11C44.html before declaring there is no dead zone. See figure 11. Rick N6RK "Avery Fineman" wrote in message ... In article B_Htc.4677$pt3.1214@attbi_s03, "Rick Karlquist N6RK" writes: There are various fixes for the dead zone problem. In the mid-1970's, Fairchild (the original company) sold an "11C44" phase detector that got rid of the dead zone by injecting a narrow pulse so that the phase detector pulses would never have to try to go to zero width. Eric Breeze holds the patent on this technique; if interested read his patent. Analog Devices makes that AD9901 phase detector which gets around the dead zone by first dividing the frequency by 2. However, it is not suitable for a frequency synthesizer because of the large spurious sidebands resulting from this technique. Motorola had some patents on the circuits in its MC145159 that dealt with the dead zone and sampling sidebands. It also used a divide by 2 technique, that was not documented; (we figured it out by observing the chip's output). That chip may have been inherited by On Semiconductor. It was originally developed for some division of GE. The "dead zone problem" is less a problem and more a state of mind. :-) When implemented with a charge-pump circuit (voltage & time converter to current) between the PFD and loop filter, it rather disappears into the woodwork of the whole PLL. The phase difference between signal and reference is proportional to the control voltage of the VCO producing the basic frequency. There is ALWAYS going to be a signal versus reference phase offset when the entire loop is in lock so this dreaded "dead zone problem" will only show up in a very narrow range of controlled frequency. General intuitive thought on any PLL or other synthesizer closed loop is that the relative phase between signal and reference is zero. It isn't. If it was, then the VCO could not be controlled. As a very rough indicator of VCO frequency, that signal v. reference offset phase exists for quick scope checking...when the control voltage range of the VCO is known. Good for a quick bench check. In practical terms, that dreaded "dead zone" isn't visible in a real-world example. Case in point: 23+ years ago, Rocketdyne Division of Rockwell International (now a Division of Boeing) was beginning work on a Deformable Mirror for laser work (they had a sizeable optics group) that used a 1 MHz signal out of optics to indicate the light phase error of an optical interferometer. I rigged up a 74H family phase-frequency detector circuit as the heart of that, an integrator out of that into an A-to-D converter to get a digital version for computer data manipulation. By all the careful measurement, the expected dead zone didn't show up on any graphing and the standard lab time interval counters could resolve, accurately, 2 nanoseconds using time averaging. [translates to rather less than a degree of phase error] The optical physicists had been hopping up and down about "dead zone" in meetings but the actual circuit performance didn't show it. One reason for the non-observation of any dead zone is that the digital gates forming the PFD were so lightly loaded in other-gate capacitance that their propagation delays all tended to be the same. Datasheet values of propagation delay of gates are all given as maximums, rather worst-case things with lots of pFds connected to outputs, etc. Put on half a prototype board, loaded only by other gates of the PFD and the resistor input of an op-amp integrator, the capacitance loading was minimal. [project was successful, and spawned more work on deformable mirrors] It can be an interesting academic problem to achieve a zero dead- dead zone effect in a PFD, but thats about it. When working at the comparison frequency of less than a few MHz, the PFD dead zone due to differential propagation delays of the gates disappears into the woodwork when using 74LS or faster digital families. There's plenty to be concerned about in any frequency synthesizer subsystem, but a phase-frequency detector gate structure is a very minor problem in my opinion. DDS and fractional-N loops in synthesizers have their own problems such as spurious output, but those problems can't really be traced to any PFD dead-zone effect. A PFD is wonderful as a control loop element in that it can control a VCO (of the loop) from way off the frequency and bring it into a lock phase range...from either worst- case start-up frequency. [way back in the beginning of radio time, lock loops had to use sawtooth sweep circuits to cure that start-up condition, and couldn't control beyond +/- 90 degrees of phase shift...PFDs easily handle +/-180 degrees] Len Anderson retired (from regular hours) electronic engineer person |
#18
![]() |
|||
|
|||
![]()
Let me try again to explain dead zone.
Many PLL's never experience the dead zone because the loop filter is constructed using op amps with high (10 mV) offset voltage specs. This offset forces the loop to lock up outside the dead zone. If you use a low offset op amp, and then put in an offset adjust pot to take out any residual offset from the phase detector, you can observe the spurious sidebands at the phase detection frequency null out. However, you will then find that the loop bandwidth has changed substantially, because you are in the dead zone region. The VCO will get more phase noise because the loop wanders around (like a bang-bang loop) in the dead zone, and/or the change in loop bandwidth has de-optimized the suppression of VCO noise by the PLL. I have personally observed this and other engineers I have mentored have also observed it (after first arguing with me that it wouldn't happen). By the way, the pot tweaking to null sidebands doesn't hold over temperature (no surprise) so it's still bogus even without the dead zone issue. To correct previous misinformation about the 11C44: the gates are not better matched; rather there is an extra pulse injection circuit as described in Eric Breeze's patent. This information is from a conversion with Eric Breeze 28 years ago. The 11C44 hasn't been available for many years but that was due to mismanagement of Fairchild (which was bought by National) rather than lack of merit of the 11C44. (There was a lot of great technology at Fairchild screwed up by mismanagement). Rick N6RK "Avery Fineman" wrote in message ... In article , "W3JDR" writes: Dead-zone = phase noise. Very little dead-zone = very little phase noise. Bigger dead-zone = bigger phase noise. You can interpolate the rest for yourself. I have to disagree with some of that. First of all, a "dead zone" or the almost-exactly-in-phase condition, occurs at only one VCO frequency where the control voltage sets up the frequency for that in-phase condition. Yes, at that exact frequency, there COULD be some phase noise. But, the phase noise may NOT be from this "dead zone" effect. Phase noise can come from MANY different sources. If it occurs well away from the in-same-phase "dead zone" then the phase noise is NOT caused by any "dead zone." The relative phase between signal and reference inputs to a PFD correspond to the VCO control voltage (times the charge-pump or integrator circuit constants). Signal and reference phases when in lock will always be offset from one another, one leading and one lagging. A good loop will show a constant offset of phases even when both inputs hold a constant phase. Len Anderson |
#19
![]() |
|||
|
|||
![]()
Let me try again to explain dead zone.
Many PLL's never experience the dead zone because the loop filter is constructed using op amps with high (10 mV) offset voltage specs. This offset forces the loop to lock up outside the dead zone. If you use a low offset op amp, and then put in an offset adjust pot to take out any residual offset from the phase detector, you can observe the spurious sidebands at the phase detection frequency null out. However, you will then find that the loop bandwidth has changed substantially, because you are in the dead zone region. The VCO will get more phase noise because the loop wanders around (like a bang-bang loop) in the dead zone, and/or the change in loop bandwidth has de-optimized the suppression of VCO noise by the PLL. I have personally observed this and other engineers I have mentored have also observed it (after first arguing with me that it wouldn't happen). By the way, the pot tweaking to null sidebands doesn't hold over temperature (no surprise) so it's still bogus even without the dead zone issue. To correct previous misinformation about the 11C44: the gates are not better matched; rather there is an extra pulse injection circuit as described in Eric Breeze's patent. This information is from a conversion with Eric Breeze 28 years ago. The 11C44 hasn't been available for many years but that was due to mismanagement of Fairchild (which was bought by National) rather than lack of merit of the 11C44. (There was a lot of great technology at Fairchild screwed up by mismanagement). Rick N6RK "Avery Fineman" wrote in message ... In article , "W3JDR" writes: Dead-zone = phase noise. Very little dead-zone = very little phase noise. Bigger dead-zone = bigger phase noise. You can interpolate the rest for yourself. I have to disagree with some of that. First of all, a "dead zone" or the almost-exactly-in-phase condition, occurs at only one VCO frequency where the control voltage sets up the frequency for that in-phase condition. Yes, at that exact frequency, there COULD be some phase noise. But, the phase noise may NOT be from this "dead zone" effect. Phase noise can come from MANY different sources. If it occurs well away from the in-same-phase "dead zone" then the phase noise is NOT caused by any "dead zone." The relative phase between signal and reference inputs to a PFD correspond to the VCO control voltage (times the charge-pump or integrator circuit constants). Signal and reference phases when in lock will always be offset from one another, one leading and one lagging. A good loop will show a constant offset of phases even when both inputs hold a constant phase. Len Anderson |
#20
![]() |
|||
|
|||
![]()
If you build a PLL with a low offset op amp (not the usual
ones with 10 mV offset spec) and then use a pot to tweak out the residual phase detector output offset voltage, you will see the sidebands on the VCO null out at a certain setting of the pot. At this setting, you will typically be in or near the dead zone. Although the spurious sidebands are impressively low, the loop bandwidth will now be unpredictable, which may de-optimize the phase noise. Also, there may be a lot of low frequency residual FM on the VCO because the loop is acting like a bang bang loop. Many engineers have never seen this happen, because it is unlikely to happen by accident. BTW, the pot setting won't hold very well over temperature. Rick N6RK "Avery Fineman" wrote in message ... In article , "W3JDR" writes: Dead-zone = phase noise. Very little dead-zone = very little phase noise. Bigger dead-zone = bigger phase noise. You can interpolate the rest for yourself. I have to disagree with some of that. First of all, a "dead zone" or the almost-exactly-in-phase condition, occurs at only one VCO frequency where the control voltage sets up the frequency for that in-phase condition. Yes, at that exact frequency, there COULD be some phase noise. But, the phase noise may NOT be from this "dead zone" effect. Phase noise can come from MANY different sources. If it occurs well away from the in-same-phase "dead zone" then the phase noise is NOT caused by any "dead zone." The relative phase between signal and reference inputs to a PFD correspond to the VCO control voltage (times the charge-pump or integrator circuit constants). Signal and reference phases when in lock will always be offset from one another, one leading and one lagging. A good loop will show a constant offset of phases even when both inputs hold a constant phase. Len Anderson |
Reply |
Thread Tools | Search this Thread |
Display Modes | |
|
|
![]() |
||||
Thread | Forum | |||
Phase differences in direct conversion receivers | Homebrew | |||
V and I not in phase at resonance Frequency in RLC network? | Homebrew |