[time-nuts] Designing and building an OCXO and GPSDO

SAIDJACK at aol.com SAIDJACK at aol.com
Wed Aug 13 16:24:46 UTC 2008


Thanks Bruce,
 
it would be interesting to see how the different topologies affect phase  
noise and stability etc, and what kind of performance can be achieved.
 
bye,
Said
 
 
In a message dated 8/12/2008 20:19:03 Pacific Daylight Time,  SAIDJACK@
aol.com writes:

Hi  Bruce,

do you have any phase noise/stability measurements for  these  circuits?

thanks,
Said


In a message dated  8/12/2008 18:53:38 Pacific Daylight Time,  
bruce.griffiths at xtra.co.nz  writes:

Attached  schematic is for a variant of the Wenzel circuit  using a JFET 
high input  impedance buffer to drive a cascaded pair of  CB stages.

L104 is  approximately resonant with C111 at 3MHz so  that either an RF 
choke and  series resistor or a relative;y low  value resistor (10K) can 
be used to  set the JFET gate  voltage.
The impedance of C104 at 3MHz is about 530 ohms  so a 1mA  crystal current 
will result in about 530 mV rms across  C104.
An  additional inductor can be used in series with the crystal to   
resonate out the input capacitance of the oscillator stage if  required,  
this will allow a greater tuning range to be  achieved.

Inductor  L104  needs to have a reasonably high Q (  > 100 @ 3MHz) to 
avoid  degrading the loaded  Q  significantly.

The drain current of JFET  Q103 is determined by  the collector current of 
Q104 this minimises the  effect of JFET  parameter variations from part to 
part on its drain   current.

The RF voltage at the source of Q103 can be amplified (a   widebandwidth 
opamp could be used) and used to drive a detector diode  for  AGC purposes.
Alternatively a common base stage connected to the  other end  of the 
secondary of T101 could be used an RF current  source to drive a  full 
wave diode detector with a low load  resistance.
This will largely  eliminate the effect of the detector  diode forward 
voltage drops on the  detected output. This detector dc  load current can 
than be compared with a  reference current and the  dc collector current 
of Q101 adjusted to  regulate the crystal  current.

Bruce




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7  )


Hi Bruce,



do you have  any phase noise/stability measurements for these  circuits?



thanks,
Said



In a message dated 8/12/2008 18:53:38 Pacific  Daylight Time,
bruce.griffiths at xtra.co.nz  writes:

Attached schematic is for a variant of the  Wenzel circuit using a
JFET
high  input impedance buffer to drive a cascaded pair of CB stages.
L104 is approximately resonant with C111 at 3MHz so that either  an
RF
choke and series resistor  or a relative;y low value resistor (10K)
can
be used to set the JFET gate voltage.
The  impedance of C104 at 3MHz is about 530 ohms so a 1mA crystal
current
will result in about 530 mV rms  across C104.
An additional inductor can be used in  series with the crystal to
resonate out the input  capacitance of the oscillator stage if
required,
this will allow a greater tuning range to be  achieved.
Inductor L104  needs to have a  reasonably high Q ( > 100 @ 3MHz) to
avoid degrading  the loaded  Q significantly.
The drain current of  JFET Q103 is determined by the collector
current  of
Q104 this minimises the effect of JFET parameter  variations from
part to
part on  its drain current.
The RF voltage at the source of Q103  can be amplified (a
widebandwidth
opamp could be used) and used to drive a detector diode for  AGC
purposes.
Alternatively a  common base stage connected to the other end of the
secondary of T101 could be used an RF current source to drive a full
wave diode detector with a low load resistance.
This will largely eliminate the effect of the detector diode  forward
voltage drops on the detected output. This  detector dc load current
can
than be compared with a reference current and the dc collector
current
of Q101 adjusted to regulate the  crystal current.
Bruce
[cid:X.MA1.1218597403 at aol.com]
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reviews on AOL  Autos.

References

1.  
http://autos.aol.com/cars-BMW-128-2008/expert-review?ncid=aolaut00050000000017




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and follow the  instructions there.




**************Looking for a car that's sporty, fun and fits in your budget? 
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-------------- next part --------------
   Thanks Bruce,



   it would be interesting to see how the different topologies affect
   phase noise and stability etc, and what kind of performance can be
   achieved.



   bye,

   Said



   In a message dated 8/12/2008 20:19:03 Pacific Daylight Time,
   SAIDJACK at aol.com writes:

     Hi Bruce,
     do you have any phase noise/stability measurements for these
     circuits?
     thanks,
     Said
     In a message dated 8/12/2008 18:53:38 Pacific Daylight Time,
     bruce.griffiths at xtra.co.nz writes:
     Attached  schematic is for a variant of the Wenzel circuit using a
     JFET
     high input  impedance buffer to drive a cascaded pair of CB stages.
     L104 is  approximately resonant with C111 at 3MHz so that either an
     RF
     choke and  series resistor or a relative;y low value resistor (10K)
     can
     be used to  set the JFET gate voltage.
     The impedance of C104 at 3MHz is about 530 ohms  so a 1mA crystal
     current
     will result in about 530 mV rms across  C104.
     An additional inductor can be used in series with the crystal to
     resonate out the input capacitance of the oscillator stage if
     required,
     this will allow a greater tuning range to be achieved.
     Inductor  L104  needs to have a reasonably high Q ( > 100 @ 3MHz) to
     avoid  degrading the loaded  Q significantly.
     The drain current of JFET  Q103 is determined by the collector
     current of
     Q104 this minimises the  effect of JFET parameter variations from
     part to
     part on its drain  current.
     The RF voltage at the source of Q103 can be amplified (a
     widebandwidth
     opamp could be used) and used to drive a detector diode for  AGC
     purposes.
     Alternatively a common base stage connected to the other end  of the
     secondary of T101 could be used an RF current source to drive a
     full
     wave diode detector with a low load resistance.
     This will largely  eliminate the effect of the detector diode
     forward
     voltage drops on the  detected output. This detector dc load current
     can
     than be compared with a  reference current and the dc collector
     current
     of Q101 adjusted to  regulate the crystal current.
     Bruce
     _______________________________________________
     time-nuts  mailing list -- time-nuts at febo.com
     To unsubscribe, go to
     https://www.febo.com/cgi-bin/mailman/listinfo/time-nuts
     and follow the  instructions there.
     **************Looking for a car that's sporty, fun and fits in your
     budget?
     Read reviews on AOL Autos.
     (http://autos.aol.com/cars-BMW-128-2008/expert-review?ncid=aolaut000
     50000000017 )
        Hi Bruce,
        do you have any phase noise/stability measurements for these
     circuits?
        thanks,
        Said
        In a message dated 8/12/2008 18:53:38 Pacific Daylight Time,
        bruce.griffiths at xtra.co.nz writes:
          Attached schematic is for a variant of the Wenzel circuit using
     a
          JFET
          high input impedance buffer to drive a cascaded pair of CB
     stages.
          L104 is approximately resonant with C111 at 3MHz so that either
     an
          RF
          choke and series resistor or a relative;y low value resistor
     (10K)
          can
          be used to set the JFET gate voltage.
          The impedance of C104 at 3MHz is about 530 ohms so a 1mA
     crystal
          current
          will result in about 530 mV rms across C104.
          An additional inductor can be used in series with the crystal
     to
          resonate out the input capacitance of the oscillator stage if
          required,
          this will allow a greater tuning range to be achieved.
          Inductor L104  needs to have a reasonably high Q ( > 100 @
     3MHz) to
          avoid degrading the loaded  Q significantly.
          The drain current of JFET Q103 is determined by the collector
          current of
          Q104 this minimises the effect of JFET parameter variations
     from
          part to
          part on its drain current.
          The RF voltage at the source of Q103 can be amplified (a
          widebandwidth
          opamp could be used) and used to drive a detector diode for AGC
          purposes.
          Alternatively a common base stage connected to the other end of
     the
          secondary of T101 could be used an RF current source to drive a
     full
          wave diode detector with a low load resistance.
          This will largely eliminate the effect of the detector diode
     forward
          voltage drops on the detected output. This detector dc load
     current
          can
          than be compared with a reference current and the dc collector
          current
          of Q101 adjusted to regulate the crystal current.
          Bruce
          [cid:X.MA1.1218597403 at aol.com]
          _______________________________________________
          time-nuts mailing list -- time-nuts at febo.com
          To unsubscribe, go to
          https://www.febo.com/cgi-bin/mailman/listinfo/time-nuts
          and follow the instructions there.

     __________________________________________________________________
        Looking for a car that's sporty, fun and fits in your budget?
     [1]Read
        reviews on AOL Autos.
     References
        1.
     http://autos.aol.com/cars-BMW-128-2008/expert-review?ncid=aolaut0005
     0000000017
     [cid:X.MA1.1218644679 at aol.com]
     _______________________________________________
     time-nuts mailing list -- time-nuts at febo.com
     To unsubscribe, go to
     https://www.febo.com/cgi-bin/mailman/listinfo/time-nuts
     and follow the instructions there.
     __________________________________________________________________

   Looking for a car that's sporty, fun and fits in your budget? [1]Read
   reviews on AOL Autos.

References

   1. http://autos.aol.com/cars-BMW-128-2008/expert-review?ncid=aolaut00050000000017
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