Re: [time-nuts] 510 doubler

2015-02-05 Thread Fuqua, Bill L
  Ok, lets get real  here. 
Temperature variations, could cause a phase shift but a very very slow one, the 
degree would depend on the
Q of the filter, temperature coefficient of the crystal, and capacitor and how 
well it is isolated from turbulent air.
 I am not new to the game of making sensitive measurements using high Q filters.
 I would be more concerned with the phase changes due to the fractional Hz 1/f 
noise of the input threshold voltages of the FET's
also any trigger circuit that may follow used to feed counters etc in 
instruments preceding and following the doubler. I am surprised
that you aren't complaining about the sideband noise produced by the Brownian 
motion of nitrogen molecules inside the crystal case. 
  In this case it is a 2 pole filter and once the phasing capacitor is adjusted 
the only the mechanical vibrational resonance of the
crystal really counts. 
  If you are interested in High Q resonators, phase shift, etc.  you might want 
to take a look at  Review of Scientific Instruments 60, 3035 (1989),
Use of a helical resonator as a capacitive transducer in vibrating reed 
measurements where a helical resonator
is used to measure the vibrations of small crystals with an sensitivity of 
10e-7 Angstroms per square root Hertz bandwith.
  Also, take a look at citations in other papers and patents referencing this 
design.
  I just tried to describe a simple very pure sine wave doubler for your 
readers.
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Re: [time-nuts] 510 doubler

2015-02-04 Thread Andrea Baldoni
On Tue, Feb 03, 2015 at 01:12:41AM -0500, Charles Steinmetz wrote:

 transformer into a 50 ohm load, the green trace results.  This trace
 shows the simulated raw output, without any traps.  Obviously, this
 is very much closer to a clean 10MHz signal than the rectified
 signal in Figure 1.

Thank you for your explanation and graph. I got the point.
The wave shaping is very impressive.
Can you put in another graph the calculated difference to a pure sine wave?

Best regards,
Andrea Baldoni
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Re: [time-nuts] 510 doubler

2015-02-04 Thread Charles Steinmetz

Bill wrote:

Push-Push Jfet amplifier with parallel inputs and a Toroid output 
transformer, no secondary along with a simple filter using a 10 MHz 
series resonate crystal connected to one drain and an adjustable 
capacitor connected to the other would work fine. You connect the 
other ends of the two together and a loading resistor to 
ground.  The capacitor is used to neutralize or null out the shunt 
capacitance of the crystal so that a capacitive path for the other 
frequencies , 5, 15, 20, etc is eliminated.


I concur with what Bruce said regarding crystal filters (or any 
narrow bandpass filter) at the output frequency.


More fundamentally, I'm not sure I understand your description of the 
circuit.  You say it is a pair of FETs with parallel input and a 
transformer (autoformer) output.  To me, that suggests the circuit 
pictured below (one feeds the sources in parallel, the other feeds 
the gates in parallel -- it doesn't make any difference in how the 
circuit operates).


The usual push-push doubler feeds the FETs differentially, and takes 
the common-mode output.  The diagrammed circuit reverses this -- it 
feeds the FETs in parallel (common-mode) and takes the 10MHz output 
differentially.  As drawn, the circuit would have essentially no 
output at the input frequency or any of its harmonics (only that due 
to the mismatch between the FETs).  The only signals it would amplify 
are uncorrelated signals -- i.e., the FETs' input noise voltages.  A 
quick simulation confirmed no significant output at the input 
frequency or its harmonics for matched FETs.  Simulating mismatched 
FETs produced a 5MHz signal rich in harmonics, but at a very low 
level and with no suppression of the 5MHz and its odd harmonics.


I assume I misinterpreted your description and that you had a 
different circuit in mind, or that if you did have this circuit in 
mind I'm missing something about its operation.  Can you please 
describe again what you had in mind, and how it generates 10MHz?


Best regards,

Charles

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Re: [time-nuts] 510 doubler

2015-02-04 Thread Charles Steinmetz

Andrea wrote:


Can you put in another graph the calculated difference to a pure sine wave?


I'm not sure what you mean by the calculated difference to a pure 
sine wave.  I already reported the amplitudes of all of the visible 
spurs (that is, the ones above the simulation noise floor), which 
define the departure from a pure 10MHz sine wave.  I am attaching 
below the simulated spectrum analysis from which I took those 
reported amplitudes, if that helps.  (There is no new data here, it 
is just graphical rather than tabular.)


Again, this is from a simulation, and I purposely introduced 10mV of 
gate imbalance to model imperfectly-matched FETs.  It is the raw 
output from the doubler, with no traps installed.  The breadboard 
circuit performs similarly, although the 5MHz and 15MHz components 
are about 10dB lower from the breadboard than they are shown in this 
simulation (this depends on how well matched the FETs are -- I was 
able to get a better balance in real life than the imbalance I 
purposely introduced for this simulation).


Best regards,

Charles

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Re: [time-nuts] 510 doubler

2015-02-03 Thread Bruce Griffiths
Unfortunately that approach degrades the phase noise floor due to crystal 
dissipation limitations as well as degrading the phase  noise in the flicker 
region due to the crystal itself,Not only is a clean (harmonic and subharmonic 
free) sine wave desirable so is  low phase noise.Thermal drift of the crystal 
filter phase shift will also be problematic.Cascaded low Q filters suffer less 
from this  than a single high Q filter.
A low pass filter combined with series resonant shunt traps will have fewer 
issues with phase instability at 10MHz than using a 10MHz bandpass filter.

Bruce
 

 On Wednesday, 4 February 2015 9:53 AM, Fuqua, Bill L wlfuq...@uky.edu 
wrote:
   

   Push-Push Jfet amplifier with parallel inputs and a  Toroid output 
transformer, no secondary along with a
simple filter using a 10 MHz series resonate crystal connected to one drain and 
an adjustable capacitor connected
to the other would work fine. You connect the other ends of the two together 
and a loading resistor to ground.
  The capacitor is used to neutralize or null out the shunt capacitance of the 
crystal so that a capacitive path 
for the other frequencies , 5, 15, 20, etc is eliminated. Then follow up with 
your linear class A amplifier.
  The loading on the output of the crystal filter will determine it's Q and is 
not real critical, but should be
perhaps around 10-100 times the series resistance of the crystal. Since most 
readily available crystals
are not exactly on frequency a lower Q, higher R would be desired, but that 
will not greatly affect the 
5 MHz or undesired harmonic attenuation.  Perhaps one or two kHz bandpass would 
be just about right.
 Just don't overdrive the crystal. Also, for the price of $1 or less you may 
get 10 or so for further experimentation.
This combination of doubler and crystal filter should provide a very nice 
sinewave output
73
Bill wa4lav
 
 
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Re: [time-nuts] 510 doubler

2015-02-03 Thread Bruce Griffiths
Whilst the output signal of the barely class A JFET amplifier has a lower 
unwanted harmonic content and thus requires less filtering to achieve a 
given suppression of unwanted harmonics and/or subharmonics, the 
question of the flicker phase noise penalty incurred by the barely class A 
amplifier approach remains unresolved.


Bruce
On Tuesday, February 03, 2015 01:12:41 AM Charles Steinmetz wrote:
 Andrea  wrote:
 But, what is the advantage between it and a couple of diode-
connected
 transistors with a full A-class (more linear, so less spurs)
 amplifier in front
 of it?
 
 If it's so, why use a nonlinear (or barely linear) gain stage to rectify?
 Using just one stage means in general less phase noise output (but 
with
 probably more spurs that can be filtered out), versus a more stage 
linear
 amplifier (perhaps with strong negative feedblack) followed by a
 rectifier?
 
 I replied:
 The barely Class A push-push doubler does not rectify the signal
 -- it creates the second harmonic because of the primarily
 second-order transfer characteristics of the JFETs.  The design goal
 is to map the DC bias and the input signal to the portion of the
 FETs' characteristic curve that has the best fit to a second-order
 transfer function, while at the same time holding noise below the
 design requirement.
 
 Perhaps some pictures would be helpful (see below).  Figure 1 (top)
 shows an ideal full-wave rectified sine wave, similar to what is
 produced by a full-wave diode rectifier, a bipolar transistor
 push-push doubler, or a FET doubler driven into pinchoff (Class
 B).  Obviously, it is extremely rich in harmonics.  The second
 harmonic of the output (doubled) frequency is only 14dB below the
 desired signal, and a series of even harmonics stretches as far as
 the eye can see, diminishing only very slowly with increasing
 harmonic number.  (In practice, there will be a HF rolloff that makes
 things slightly better.  However, there will also be odd-order
 components, which an ideal full-wave rectifier would not produce.)
 
 Figure 2 (bottom) shows waveforms from the simulation of my barely
 Class A push-push doubler, using a matched pair of J111 FETs (J310s
 perform almost identically, with the appropriate change in the bias
 resistor).  I purposely introduced a 10mV gate voltage imbalance in
 the simulation to model imperfect matching.  The red and magenta
 traces are the currents in the two FETs, showing a primarily
 second-order transfer characteristic.  When these currents are added
 by the push-push connection and put through a 4:1 (turns ratio)
 transformer into a 50 ohm load, the green trace results.  This trace
 shows the simulated raw output, without any traps.  Obviously, this
 is very much closer to a clean 10MHz signal than the rectified signal
 in Figure 1.
 
 The 5MHz component is ~40dB below the desired 10MHz signal.  This
 depends strongly on how well the FETs are matched and on the layout
 and shielding.  J111s or J310s from the same lot, matched to within
 1mV, should do better than this (the 5MHz component from my
 breadboard circuit is below -45dBc, without any traps).  The other
 visible distortion products, and their levels, are:
 
 15MHz-75dBc
 20MHz-45dBc
 25MHz-100dBc
 30MHz-75dBc
 35MHz-100dBc   (all figures are approximate).
 
 The breadboard circuit performs similarly (the 15MHz component is
 about 10dB lower from the breadboard, so I needed traps only at 5,
 20, and 30MHz to get all spurious responses below -80dBc).
 
 As I noted before, the barely Class A circuit is not materially
 noisier than a FET push-push doubler that is run into Class AB or B,
 but it has MUCH lower spurious outputs and, therefore, does not need
 the sort of aggressive filtering the Class AB/B circuits need,
 avoiding the increase in phase noise and other problems associated
 with aggressive filters.
 
 Best regards,
 
 Charles

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Re: [time-nuts] 510 doubler

2015-02-03 Thread Charles Steinmetz

Bruce wrote:

Whilst the output signal of the barely class A JFET amplifier has a 
lower unwanted harmonic content and thus requires less filtering to 
achieve a given suppression of unwanted harmonics and/or 
subharmonics, the question of the flicker phase noise penalty 
incurred by the barely class A amplifier approach remains unresolved.


I posted the resolution a few days ago.

As I said then, I adjusted the bias and input parameters of my 
breadboard doubler to match the conditions under which the FETs are 
operated in the doubler posted on your site, and measured the change 
in noise (including in the flicker region).  The noise decreased by a 
fraction of a dB.  Accordingly, I conclude that the barely class A 
doubler's noise, including flicker noise, is within a fraction of a 
dB of a Class AB doubler using the same FETs that you consider optimized.


I also explained then why this result should come as no surprise (one 
FET in a Class AB or B doubler will not be contributing noise when it 
is cut off -- but that coincides with the other FET being at or near 
full current, so the total noise is dominated by the noise of the 
full-current FET and the benefit due to the cut-off FET is insignificant).


There may be quieter FETs with lower flicker noise corners available 
that have similar medium-cutoff characteristics and are, therefore, 
suitable for this use -- but for the reasons I have given, I believe 
that similar relative noise relationships between barely Class A and 
Class AB doublers using such FETs would hold for them, as 
well.  NOTE:  For anyone simulating JFET circuits, be aware that many 
available JFET models do not model flicker noise at all, and many of 
those that do are wildly inaccurate at simulating noise in the 
flicker region.  As always, there is no substitute for building and 
measuring the circuit.


Best regards,

Charles



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Re: [time-nuts] 510 doubler

2015-02-03 Thread Charles Steinmetz

Andrea  wrote:


But, what is the advantage between it and a couple of diode-connected
transistors with a full A-class (more linear, so less spurs) 
amplifier in front

of it?



If it's so, why use a nonlinear (or barely linear) gain stage to rectify?
Using just one stage means in general less phase noise output (but with
probably more spurs that can be filtered out), versus a more stage linear
amplifier (perhaps with strong negative feedblack) followed by a rectifier?


I replied:

The barely Class A push-push doubler does not rectify the signal 
-- it creates the second harmonic because of the primarily 
second-order transfer characteristics of the JFETs.  The design goal 
is to map the DC bias and the input signal to the portion of the 
FETs' characteristic curve that has the best fit to a second-order 
transfer function, while at the same time holding noise below the 
design requirement.


Perhaps some pictures would be helpful (see below).  Figure 1 (top) 
shows an ideal full-wave rectified sine wave, similar to what is 
produced by a full-wave diode rectifier, a bipolar transistor 
push-push doubler, or a FET doubler driven into pinchoff (Class 
B).  Obviously, it is extremely rich in harmonics.  The second 
harmonic of the output (doubled) frequency is only 14dB below the 
desired signal, and a series of even harmonics stretches as far as 
the eye can see, diminishing only very slowly with increasing 
harmonic number.  (In practice, there will be a HF rolloff that makes 
things slightly better.  However, there will also be odd-order 
components, which an ideal full-wave rectifier would not produce.)


Figure 2 (bottom) shows waveforms from the simulation of my barely 
Class A push-push doubler, using a matched pair of J111 FETs (J310s 
perform almost identically, with the appropriate change in the bias 
resistor).  I purposely introduced a 10mV gate voltage imbalance in 
the simulation to model imperfect matching.  The red and magenta 
traces are the currents in the two FETs, showing a primarily 
second-order transfer characteristic.  When these currents are added 
by the push-push connection and put through a 4:1 (turns ratio) 
transformer into a 50 ohm load, the green trace results.  This trace 
shows the simulated raw output, without any traps.  Obviously, this 
is very much closer to a clean 10MHz signal than the rectified signal 
in Figure 1.


The 5MHz component is ~40dB below the desired 10MHz signal.  This 
depends strongly on how well the FETs are matched and on the layout 
and shielding.  J111s or J310s from the same lot, matched to within 
1mV, should do better than this (the 5MHz component from my 
breadboard circuit is below -45dBc, without any traps).  The other 
visible distortion products, and their levels, are:


15MHz-75dBc
20MHz-45dBc
25MHz-100dBc
30MHz-75dBc
35MHz-100dBc   (all figures are approximate).

The breadboard circuit performs similarly (the 15MHz component is 
about 10dB lower from the breadboard, so I needed traps only at 5, 
20, and 30MHz to get all spurious responses below -80dBc).


As I noted before, the barely Class A circuit is not materially 
noisier than a FET push-push doubler that is run into Class AB or B, 
but it has MUCH lower spurious outputs and, therefore, does not need 
the sort of aggressive filtering the Class AB/B circuits need, 
avoiding the increase in phase noise and other problems associated 
with aggressive filters.


Best regards,

Charles

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Re: [time-nuts] 510 doubler

2015-02-03 Thread Fuqua, Bill L
  Push-Push Jfet amplifier with parallel inputs and a  Toroid output 
transformer, no secondary along with a
simple filter using a 10 MHz series resonate crystal connected to one drain and 
an adjustable capacitor connected
to the other would work fine. You connect the other ends of the two together 
and a loading resistor to ground.
  The capacitor is used to neutralize or null out the shunt capacitance of the 
crystal so that a capacitive path 
for the other frequencies , 5, 15, 20, etc is eliminated. Then follow up with 
your linear class A amplifier.
  The loading on the output of the crystal filter will determine it's Q and is 
not real critical, but should be
perhaps around 10-100 times the series resistance of the crystal. Since most 
readily available crystals
are not exactly on frequency a lower Q, higher R would be desired, but that 
will not greatly affect the 
5 MHz or undesired harmonic attenuation.  Perhaps one or two kHz bandpass would 
be just about right.
 Just don't overdrive the crystal. Also, for the price of $1 or less you may 
get 10 or so for further experimentation.
This combination of doubler and crystal filter should provide a very nice 
sinewave output
73
Bill wa4lav
 
 
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Re: [time-nuts] 510 doubler

2015-02-02 Thread Charles Steinmetz

Andrea wrote:


I see. This configuration is in effect a common gate B-class (or AB, or
barely A) amplifier and the rectification is a side effect.
But, what is the advantage between it and a couple of diode-connected
transistors with a full A-class (more linear, so less spurs) 
amplifier in front

of it?


It is the rectification that causes the gross nonlinearities, not the 
amplification.  So no matter how linear an amplifier you make, the 
diodes (or Class B or AB amplifier) will cause gross nonlinearities 
that we do not want.  Furthermore, transistors have both even- and 
odd-order distortion products, while JFETs have predominantly 
second-order products.  So JFETs naturally tend to produce the second 
harmonic, while transistors also produce the odd-order products we 
are trying to avoid (as well as higher even-order products).



I know that the circuit originates at NIST and thus there surely IS an
advantage. Are it trading more spurs (that you can cancel out with filtering)
for less phase noise (that you cannot recover anymore)?


I do not know precisely how the NIST circuit is biased, and as far as 
I know it is not general knowledge among time nuts -- so any 
substantive response would be conjecture.  I don't even know if NIST 
still uses it.  There are a few things to know -- NIST historically 
settles on something that works well enough, then sticks with it for 
a long time (until the phenomena they are trying to measure get 
distinctly better than their instruments).  NIST has lots of 
considerations besides pure performance, such as power consumption 
and fitting into old form factors, so they do not necessarily have 
the best possible solutions, even when they have just designed the 
next generation.  So, what we know for sure is that the JFET 
push-push doubler worked well enough for NIST's purposes when it was 
designed.  That does not mean improvements weren't possible.



Adding negative feedback linearize further the barely Class A amplifier; so,
it's good to sacrifice part of the gain of the push-push stage to reduce
flicker noise (and thus add less phase noise) and at the same time spurs.


But it is the natural second-order distortion of the JFETs that makes 
it a particularly good way to build a push-push doubler.  We don't 
*want* to linearize it!



If it's so, why use a nonlinear (or barely linear) gain stage to rectify?
Using just one stage means in general less phase noise output (but with
probably more spurs that can be filtered out), versus a more stage linear
amplifier (perhaps with strong negative feedblack) followed by a rectifier?


The barely Class A push-push doubler does not rectify the signal -- 
it creates the second harmonic largely because of the device 
characteristic.  The design goal is to map the bias and input to the 
portion of the FETs' characteristic curve that has the best fit to a 
second-order transfer function, while at the same time holding noise 
down below the noise budget.  That is why medium-cutoff FETs like the 
J111 and J310 are the best choices, not sharp-cutoff FETs like 2SK369 
and BF862.


Best regards,

Charles



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Re: [time-nuts] 510 doubler

2015-02-02 Thread Bruce Griffiths
Whilst input frequency related spurs can be significantly reduced with a 
suitable filter incorporating a sufficient number of series tuned traps plus 
a low pass filter, phase noise once incurred cannot be reduced by such 
means.
The ultimate measure of performance of the phase noise performance of a 
frequency doubler is the input referred residual phase noise both for the 
noise floor and the flicker phase regions.
The Wenzel JFET frequency doubler implementation (based on the NIST 
design) has a specified input referred residual phase noise of
-155dBc/Hz @ 10Hz
-178dBc/Hz @100kHz.
for a 5MHz input signal. 
http://www.wenzel.com/wp-content/uploads/LNHD.pdf

A BJT variant of the same circuit has an input referred residual phase noise 
for a 5MHz input
-159dBc/Hz @ 10Hz offset
-180dBc/Hz @ 100KHz offset
If I have interpreted Adrian's measurements correctly see:
http://www.timeok.it/files/high_performance_frequency_doublerv13.pdf.

It would be interesting to compare these figures with the measured 
residual phase noise of other frequency doublers such as Gerard's JFET 
doubler using BF862's and the proposed near class A JFET based 
frequency doubler.

Bruce 

 
On Tuesday, January 27, 2015 02:25:54 PM Charles Steinmetz wrote:
 Andrea wrote:
 Now I have some 5MHz DOCXO. I have started to experiment with them
 and I would like to build a frequency doubler.
 
   *   *   *
 
 By the way, I see that really many of the 10MHz reference out there, 
are in
 effect doubled 5MHz ones so build a doubler seems reasonable for me.
 
 One thing to watch for is the 5MHz leakage component.  If you are
 going to use the 10MHz standard for time-nuts experiments, the 5MHz
 component needs to be WAY down ( -80dBc) or you will get funny
 periodic ripples in stability plots.  Despite having two 5MHz traps,
 one recently published design suppresses the 5MHz component only
 about 52dB below the 10MHz output, and the 20MHz and 30MHz 
components
 are also only -50 to -55dB.
 
 For this reason (and some others, see discussions over the last
 several months in the archives) I prefer a doubler built with a
 quadrature hybrid coupler and a balanced mixer.  There is a write-up 
here:
 
 
http://www.ko4bb.com/manuals/download.php?file=02_GPS_Timing/4_App_
Notes_an
 d_Articles/Frequency_doubler_quadrature_DBM.pdf
 
 I recently revived an old, stalled project to develop a JFET
 push-push doubler for use at 5MHz (see schematic below).
 
 FETs with very high transconductance and very small pinchoff voltage
 (what a tube designer would call a sharp cutoff characteristic)
 (e.g., 2SK369, BF862, etc.) are attractive on first look because they
 can operate with lower conversion loss or even some conversion
 gain.  However, they are not well suited for doubler duty for two
 reasons: (i) their characteristics have a very short range of
 2nd-order curvature, so in order to keep noise down they must be
 driven into regions of higher-order distortion and therefore generate
 lots of spurious energy; and (ii) they are devilishly hard to match
 well enough to suppress the input frequency feedthrough.  Note that
 you also need to put enough voltage on the FET drains to get them
 well into the saturation region -- a Vcc of 5v is not enough.  Again,
 the penalty is lots of spurious energy.  So, the lower conversion
 loss of sharp-cutoff FETs is not the benefit it might at first appear
 to be -- it is much easier to add gain after the doubler than to
 remove unwanted spurious mixing products.
 
 The design below uses medium-cutoff FETs and a Vcc of 15v (I found
 that J111 and J310 work best and can be matched sufficiently with a
 one-point match; 2N4416 and others also work, but are fussier and
 would benefit from a 2- or 3-point match).  At an input of 500mVrms,
 their long 2nd-order characteristic is used efficiently to generate
 10MHz with relatively little spurious energy.
 
 I had no problem finding one or more FET pairs matched to within 1mV,
 given 20 devices from the same lot (YMMV).  With properly adjusted
 traps at 5, 20, and 30MHz, all spurious responses were below
 -80dBc.  The inductors can be commercial RF parts with Q of 200 or so
 (I used some high-quality through-hole RF inductors I had on hand --
 I doubt any SMD inductors will work).  The trap capacitors should be
 C0G/NP0 ceramics for the bulk of the capacitance, plus very small
 trimmers (I used 27pF, 27pF, and 100pF plus 0.2--6pF glass piston
 trimmers).  I wound the two transformers on Mix-61 toroid cores (each
 winding is 20 turns on a FT37-61 core -- the inductance is a little
 lower than called out).  Mini-Circuits parts (or equivalents) may also 
work.
 
 Best regards,
 
 Charles

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Re: [time-nuts] 510 doubler

2015-02-01 Thread Bruce Griffiths
Not a good idea to use a bandpass filter even a crystal filter as such a filter 
has a relatively large phase shift tempco.The flicker phase noise of the filter 
crystal will degrade the output signal flicker phase noise 
significantly.Another issue is that the maximum crystal current will limit the 
maximum signal input to the crystal filter and thus degrade the output phase 
noise floor over that achievable using other approaches.

Bruce
 

 On Wednesday, 28 January 2015 11:19 PM, Alberto di Bene dib...@usa.net 
wrote:
   

 On 1/27/2015 11:57 PM, Bruce Griffiths wrote:

 /The only viable solution is to use better filtering of the output of a 
 switching multiplier./

What about filtering the doubler output with a 10 MHz xtal ?

73  Alberto  I2PHD



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Re: [time-nuts] 510 doubler

2015-01-31 Thread Andrea Baldoni
On Fri, Jan 30, 2015 at 07:35:34PM +0100, Gerhard Hoffmann wrote:

 As usual, it depends. If you want absolutely deep notches, it is
 easy with the usual molded chokes
 to produce craters at 5 and 15 MHz that meet at 10 MHz, even
 producing some loss there.

Hello.
Let me sum up everything and please correct me:

the square-law characteristic of devices should be avoided, so the
configuration of the doubler must be some sort of ideal full wave rectifier

it's better to use diode-connected transistors like the 2N because they are
less noisy than Schottky diodes at frequency  40MHz (what about the normal
P-N diodes?)

matching is very important, so monolithic doubles or quadruples could be the
right choice, provided their other characteristics are compatible and the
substrate connection is not a problem

bandpass filtering must be avoided because of added unwanted
temperature-dependent phase shifts, so harmonic suppression should be obtained
by notch filtering

the notch filters could be made using quartz resonators but their high
impedance versus LC ones should be taken into account and, anyway, it's
difficult to find exactly tuned quartz (particularly for the higher harmonics
because of the overtone cut) - the sharpness of quartz filtering is not needed
anyway because the harmonics are distant enough for LC filters (what about
ceramic resonators?)

I add some questions.
I saw that most of the doublers out there are using a center tapped transformer
to obtain +-180 while the Racal circuit use a single ended input / balanced
output transistor discrete differential amplifier, thus combining phase
splitting with gain and impedance matching (but not isolation).
That configuration should be avoided because the transformer is normally a
better matched splitter?
On the base of many considerations, the Racal circuit is flawed in many parts;
it's anyway good enough for the counters it was designed for or the better
performance of other doublers will show up?

Best regards,
Andrea Baldoni
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Re: [time-nuts] 510 doubler

2015-01-31 Thread Charles Steinmetz

I wrote:

In both cases, when the FETs are conducting they are operating as 
common-source linear amplifiers, NOT as switches.


should be, common gate linear amplifiers

Best regards,

Charles



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Re: [time-nuts] 510 doubler

2015-01-30 Thread Richard (Rick) Karlquist

On 1/29/2015 5:41 PM, Alexander Pummer wrote:

And the narrow notch for the harmonic is not required anyway, since the
fundamental is fare enough, therefore a high Q  LC trap will work
better, also with the setting of the biasing af the active devices the

Alex KJ6UHN


When I designed the 5071A RF chain, I used five cascaded frequency
doublers to go from 10 MHz to 320 MHz.  I definitely used traps
to reduce the 10, 30, and 40 MHz spurs (using 10-20 MHz as an
example).  It was no easy thing because I could only use coils of 
moderate Q (less than 50) and I needed at least 80 dB suppression.  You 
might wonder why I needed to reduce 40 MHz spurs in the 20 MHz

output.  It turns out (little known fact) that the if I drove
the 20-40 MHz doubler with 20 MHz contaminated with 40 MHz
harmonics, it would degrade the spectral purity of the 40 MHz
output.  Strange but true.

The 5071 filters are basically cascaded notch filters, as
opposed to band pass filters.  Doing this allowed me to
have zero adjustments.  Previous atomic clocks used narrow
high-Q filters that had to be tuned up, and were temperature
sensitive.  The production engineers had to constantly stay
on top of these filters because they were so temperamental.
OTOH, the 5071 filters just work.  There was never even a
production change to them AFAIK.  The key to getting the notch
filters to work was to use 2% components, and use two coils
and or two capacitors together to get around the fact that
the standard values are quantized to 10%.  Additionally, I
measured each tank circuit in situ on the PC board and tweaked
it to take into account the de facto board parasitics.

Rick Karlquist N6RK
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Re: [time-nuts] 510 doubler

2015-01-30 Thread Gerhard Hoffmann

Am 30.01.2015 um 02:41 schrieb Alexander Pummer:
And the narrow notch for the harmonic is not required anyway, since 
the fundamental is fare enough, therefore a high Q  LC trap will work 
better, also with the setting of the biasing af the active devices the 
spures could be reduced to [ just observe the output with a spectrum 
analyzer and set the bias of one site to minimum harmonics, there will 
be no common optimum for all harmonics, but a good compromise could be 
achieved ]
As usual, it depends. If you want absolutely deep notches, it is easy 
with the usual molded chokes
to produce craters at 5 and 15 MHz that meet at 10 MHz, even producing 
some loss there.

The harmonics are gone, then.

At the -3dB point of a resonator we have 45° phase shift, now calculate 
how many ps delay that

is at 10 MHz and then speculate on temperature stability.

On MY doubler board, Amidon toroids are in the layout, too, and I have 
written that they are good enough.
They are hard to get. I have heard that Amidon is really Micrometals, 
but have no cross
reference. A good alternative would be Siemens K1 pot cores, but they 
are much too big and probably only NOS.

But everybody can get 5 and 15 MHz crystals for 35 cents.



BTW, this is the spectrum of a Morion MV89A that happenes to be on my table:
 
https://picasaweb.google.com/lh/photo/4UEjkc8uy_vkE5nTUR0BEdMTjNZETYmyPJy0liipFm0?feat=directlink 


10 dB external attenuator.  Could use some filtering, too.


regards, Gerhard

ps
My two  BF862 are quite different. delta Vsource = 100mV.
Changing that would be the cheapest improvement.



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Re: [time-nuts] 510 doubler

2015-01-30 Thread Alexander Pummer
And the narrow notch for the harmonic is not required anyway, since the 
fundamental is fare enough, therefore a high Q  LC trap will work 
better, also with the setting of the biasing af the active devices the 
spures could be reduced to [ just observe the output with a spectrum 
analyzer and set the bias of one site to minimum harmonics, there will 
be no common optimum for all harmonics, but a good compromise could be 
achieved ]

73
Alex KJ6UHN
On 1/29/2015 2:16 PM, Richard (Rick) Karlquist wrote:



On 1/28/2015 11:28 AM, Charles Steinmetz wrote:

Gerhard wrote:


It is a different game when you want to notch away sub/harmonics.


One problem with using crystals as traps (notch filters) is that the
series resistance of a crystal is several orders of magnitude higher
than that of a good series-resonant LC -- generally in the 50-100 ohm
range.  So, although the notch is very narrow, it will not be very deep
unless it is in a high-impedance circuit.  For example, in a 50 ohm


It is very straightforward to use LC networks to transform the
impedance of the crystal to a much lower value and get around this
problem.

Rick Karlquist N6RK
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Re: [time-nuts] 510 doubler

2015-01-29 Thread Charles Steinmetz
I had forgotten about one quite promising candidate -- the THAT300 
matched monolithic quad.  I have some of those, too.  I'll put it on 
the to-do list.  To the best of my knowledge, they do not have 
reverse protection diodes across the B-E junctions (I've never had 
any reason to check).


Best regards,

Charles




I wrote:

Once upon a time, Motorola made monolithic quad BJTs -- but I'm 
not aware of any matched quads similar to 2Ns at this time.


Gerhard replied:


There still are
MAT04
HFA3046-3096-3127-3128

if duals are enough:
SSM2220
MAT12
also mat02, mat03, maybe SSM2110 [probably meant SSM2210?  also, 
there is SSM2212]


I had thought of these, but unfortunately, all of the AD parts (MAT 
and SSM) -- which otherwise look promising -- have reverse diodes 
across the B-E junctions, which rules them out as diode substitutes.


The HFA parts are small-geometry, ultra-high frequency devices (Ft = 
8GHz for the NPNs), not at all like 2Ns.  It is doubtful they 
would have the low flicker noise of s.  They are monolithic, so 
they should be pretty well matched, but only the differential pair 
in the 3046 is actually specified for matching -- and you couldn't 
use both of the diff pair in a ring structure because of the common 
cathodes.  The 3127 would be the part to try.  I have some, so maybe 
I'll try them (but I'm not hopeful).


Best regards,

Charles




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Re: [time-nuts] 510 doubler

2015-01-29 Thread Richard (Rick) Karlquist



On 1/28/2015 11:28 AM, Charles Steinmetz wrote:

Gerhard wrote:


It is a different game when you want to notch away sub/harmonics.


One problem with using crystals as traps (notch filters) is that the
series resistance of a crystal is several orders of magnitude higher
than that of a good series-resonant LC -- generally in the 50-100 ohm
range.  So, although the notch is very narrow, it will not be very deep
unless it is in a high-impedance circuit.  For example, in a 50 ohm


It is very straightforward to use LC networks to transform the
impedance of the crystal to a much lower value and get around this
problem.

Rick Karlquist N6RK
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Re: [time-nuts] 510 doubler

2015-01-28 Thread Alberto di Bene

On 1/27/2015 11:57 PM, Bruce Griffiths wrote:


/The only viable solution is to use better filtering of the output of a 
switching multiplier./


What about filtering the doubler output with a 10 MHz xtal ?

73  Alberto  I2PHD



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Re: [time-nuts] 510 doubler

2015-01-28 Thread Charles Steinmetz

Bruce wrote:

Using the square law characteristic will inevitably increase the 
phase noise floor particularly in the flicker region with respect to 
just using the switching characteristic of a JFET, diode or 
BJT  (non saturated).


Even FETs with very large transconductance and low pinchoff voltage 
do not switch cleanly in a push-push mixer -- there is always plenty 
of square-law behavior to add flicker noise.  So the difference is 
not really all that great.  Furthermore, in practice whatever 
difference there is will be swamped in many (if not most) cases faced 
by amateur time nuts by the much larger phase noise of their sources.


There are always tradeoffs.

The only viable solution is to use better filtering of the output of 
a switching multiplier.


For the reasons given above, I disagree that a switching multiplier 
is the only viable solution for amateur time nuts.  For NIST, 
possibly.  But not for amateur time nuts.  Given a dirty multiplier 
such as a push-push doubler with 2SK369s or BF862s, the only way to 
get the fundamental and distortion products at 30MHz and below down 
to suitable levels for critical work is to use a high-Q 10MHz filter 
plus a series of traps.  The high-Q 10MHz filter brings its own low 
frequency stability problems.


There are always tradeoffs.

If you intend to use a diode ring based mixer configuration diode 
connected (collector shorted to base) npns such as 2N222's are 
significantly quieter (as shown by NIST) than schottky diodes for 
frequencies below 40MHz or so.


Yes, that is well known.  However, the transistors need to be well 
matched or, once again, you end up with spurious products that are 
hard to remove without causing collateral damage.  (I speak from 
experience -- I have built mixers that way.)  This is mitigated to a 
large extent with matched diode rings as used in diode DBMs.  The 
advantage at 10Hz with 2Ns is only 2 or 3 dB over a good Schottky 
ring, so unless one is comparing better sources than most amateur 
time nuts have access to, it will be lost in the source noise (note 
also that there is a crossover, above which the s are about 10dB 
worse).  Given the relatively small potential gain and the effort 
required to match four 2Ns to sufficient accuracy not to do more 
harm than good, I believe this is an exercise best left to those who 
know they need the modest advantage (again, not many of us amateur 
time nuts).  Once upon a time, Motorola made monolithic quad BJTs -- 
but I'm not aware of any matched quads similar to 2Ns at this 
time.  [Several manufacturers still claim to make MPQs, but those 
are not monolithic and not matched.]


There are always tradeoffs.

Notwithstanding theoretical objections, the described circuit works 
very nicely and performs substantially better than most time nuts 
need.  I presume that when one is willing to afford sources that 
require better performance, one will (1) know that, and (2) also be 
willing to afford an expensive doubler that meets that need.


Best regards,

Charles



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Re: [time-nuts] 510 doubler and old Toko RF catalogue (Cirkit2nd ed. 1994)

2015-01-28 Thread David

Andrea, an answer your original Toko data question  below.

Message: 12
Date: Tue, 27 Jan 2015 16:53:07 +0100
From: Andrea Baldoni erm1ea...@ermione.com
To: time-nuts@febo.com
Subject: [time-nuts] 510 doubler and old Toko RF catalogue (Cirkit2nd
ed.1994)

 cut some stuff

Finally I found that a (fairly) complete Toko catalog existed, it was
sold by
Cirkit in '94 and it's not available anymore.
Someone has it in PDF form, or want to borrow it to me to scan it?
Best regards,
Andrea Baldoni

I had a look at the BEC catalogues and they have the same Toko data,
rather than scan 60 pages or so. You can get what you want with the
WayBack machine (web archive) to see old Toko data online right now at
the archived  www.bec.co.uk site, try this for a starter:

http://web.archive.org/web/20041129173623/http://217.34.228.137/PG800/8var/p25.htm

I think BEC (Bonex Electronic Components) followed on from CirKit but
don't remember if there was a formal connection between the companies or 
not.


Hope that helps, this method to find old data is frequently.

David
--


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Re: [time-nuts] 510 doubler

2015-01-28 Thread Gerhard Hoffmann

Am 28.01.2015 um 00:59 schrieb Alberto di Bene:

On 1/27/2015 11:57 PM, Bruce Griffiths wrote:

/The only viable solution is to use better filtering of the output of 
a switching multiplier./


What about filtering the doubler output with a 10 MHz xtal ?

73  Alberto  I2PHD


In a correctly designed oscillator, the close-in phase noise
is determined by the crystal only and it's generally accepted
that there are 20 dB differences from a single batch. Our
data support that. Only 10% are really good.

If you filter with a crystal that is in resonance it will impress
its own phase noise on the signal-to-be-filtered, and the odds
are that you lose.

Also, crystal dissipation should be only in the 100s of uW max.
Using it to filter a 10 dBm signal probably will do harm.

It is a different game when you want to notch away sub/harmonics.
The power levels of the harmonics are much lower and the
crystal does not resonate on the resonator frequency. If you
mis-tune a trap, it won't deliver its notch but it will leave all other
frequencies alone. A LC series circuit that produces a crater of
15 % center frequency could have more global effects if mis-aligned.

When playing with the notch filters for my doubler I got the idea
that one could use them to filter away sideband noise even at the
16 dBm level. One would have to be careful not to tune a notch
over the carrier, but stay away 100 Hz to some KHz. That might
bring an oscillator from quite good to impressive over a limited
offset range. I have made a filter board for a dozen notch crystals.
That could be populated with the 90% losers from oscillator production.

There is also an offset generator from JPL IIRC where they divide
100 MHz down to 10 KHz, subtract that from the 100 MHz with a
single sideband mixer and use the 99.99 MHz for a DMTD system.
Here one could use the notch filter array to get rid of the
residual carrier  wrong sideband.  DDS-free.

But I have no time to follow that in the moment. :-(

73, Gerhard, DK4XP


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Re: [time-nuts] 510 doubler and old Toko RF catalogue (Cirkit2nd ed. 1994)

2015-01-28 Thread Adrian Godwin
I think another spinoff from Cirkit was Mainline Electronics of Leicester.
They also mostly disappeared (though I have wondered if they still trade as
the ebay seller anonalouise, who seems to have similar stock).

Mainline Electronics seems to exist as a Russian website, and it looks as
though they have something similar to the Toko range :

http://mainline-group.ru/product-category/coil_transform/moulded/


Barend Hendrikson http://barendh.home.xs4all.nl/Indexeng.htm also has a
useful range of RF components.


On Wed, Jan 28, 2015 at 10:00 AM, David t_list_1_o...@braw.co.uk wrote:

 Andrea, an answer your original Toko data question  below.

 Message: 12
 Date: Tue, 27 Jan 2015 16:53:07 +0100
 From: Andrea Baldoni erm1ea...@ermione.com
 To: time-nuts@febo.com
 Subject: [time-nuts] 510 doubler and old Toko RF catalogue (Cirkit2nd
 ed.1994)

  cut some stuff

 Finally I found that a (fairly) complete Toko catalog existed, it was
 sold by
 Cirkit in '94 and it's not available anymore.
 Someone has it in PDF form, or want to borrow it to me to scan it?
 Best regards,
 Andrea Baldoni

 I had a look at the BEC catalogues and they have the same Toko data,
 rather than scan 60 pages or so. You can get what you want with the
 WayBack machine (web archive) to see old Toko data online right now at
 the archived  www.bec.co.uk site, try this for a starter:

 http://web.archive.org/web/20041129173623/http://217.34.
 228.137/PG800/8var/p25.htm

 I think BEC (Bonex Electronic Components) followed on from CirKit but
 don't remember if there was a formal connection between the companies or
 not.

 Hope that helps, this method to find old data is frequently.

 David
 --



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 mailman/listinfo/time-nuts
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Re: [time-nuts] 510 doubler

2015-01-28 Thread Charles Steinmetz

Gerhard wrote:


It is a different game when you want to notch away sub/harmonics.


One problem with using crystals as traps (notch filters) is that the 
series resistance of a crystal is several orders of magnitude higher 
than that of a good series-resonant LC -- generally in the 50-100 ohm 
range.  So, although the notch is very narrow, it will not be very 
deep unless it is in a high-impedance circuit.  For example, in a 50 
ohm circuit (50 ohms looking each way, so 25 ohms at the node) you 
will be lucky to get 3dB of attenuation.  To get 40dB of suppression, 
the nodal impedance would need to be at least 5k ohms, perhaps 
even 10k ohms -- and the high impedance adds noise, which means 
there is a phase noise penalty.  Another problem is that the narrow 
notches are prone to sliding off frequency with small temperature changes.


Also, while a 5MHz trap crystal will almost certainly be a 
fundamental-mode resonator, that will probably not be true at, say, 
30MHz -- so a 30MHz trap would most likely have a notch at or near 
the desired output frequency.


Made with good, high-Q RF inductors (forget SM parts), an LC trap is 
generally preferable to a crystal trap.  There is still some 
temperature sensitivity, but the greater width is much more 
forgiving.  At the same time, the Q is high enough that you don't 
have to worry about effects 5MHz away when you are trapping 
frequencies of 30MHz and below.


Best regards,

Charles



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Re: [time-nuts] 510 doubler

2015-01-28 Thread Charles Steinmetz

I wrote:

Once upon a time, Motorola made monolithic quad BJTs -- but I'm not 
aware of any matched quads similar to 2Ns at this time.


Gerhard replied:


There still are
MAT04
HFA3046-3096-3127-3128

if duals are enough:
SSM2220
MAT12
also mat02, mat03, maybe SSM2110 [probably meant SSM2210?  also, 
there is SSM2212]


I had thought of these, but unfortunately, all of the AD parts (MAT 
and SSM) -- which otherwise look promising -- have reverse diodes 
across the B-E junctions, which rules them out as diode substitutes.


The HFA parts are small-geometry, ultra-high frequency devices (Ft = 
8GHz for the NPNs), not at all like 2Ns.  It is doubtful they 
would have the low flicker noise of s.  They are monolithic, so 
they should be pretty well matched, but only the differential pair in 
the 3046 is actually specified for matching -- and you couldn't use 
both of the diff pair in a ring structure because of the common 
cathodes.  The 3127 would be the part to try.  I have some, so maybe 
I'll try them (but I'm not hopeful).


Best regards,

Charles



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Re: [time-nuts] 510 doubler and old Toko RF catalogue (Cirkit2nd ed. 1994)

2015-01-28 Thread paul swed
This site is quite helpful. I happened to pick up several toko kits last
years and the data is here.
Thank you

On Wed, Jan 28, 2015 at 5:00 AM, David t_list_1_o...@braw.co.uk wrote:

 Andrea, an answer your original Toko data question  below.

 Message: 12
 Date: Tue, 27 Jan 2015 16:53:07 +0100
 From: Andrea Baldoni erm1ea...@ermione.com
 To: time-nuts@febo.com
 Subject: [time-nuts] 510 doubler and old Toko RF catalogue (Cirkit2nd
 ed.1994)

  cut some stuff

 Finally I found that a (fairly) complete Toko catalog existed, it was
 sold by
 Cirkit in '94 and it's not available anymore.
 Someone has it in PDF form, or want to borrow it to me to scan it?
 Best regards,
 Andrea Baldoni

 I had a look at the BEC catalogues and they have the same Toko data,
 rather than scan 60 pages or so. You can get what you want with the
 WayBack machine (web archive) to see old Toko data online right now at
 the archived  www.bec.co.uk site, try this for a starter:

 http://web.archive.org/web/20041129173623/http://217.34.
 228.137/PG800/8var/p25.htm

 I think BEC (Bonex Electronic Components) followed on from CirKit but
 don't remember if there was a formal connection between the companies or
 not.

 Hope that helps, this method to find old data is frequently.

 David
 --


 ___
 time-nuts mailing list -- time-nuts@febo.com
 To unsubscribe, go to https://www.febo.com/cgi-bin/
 mailman/listinfo/time-nuts
 and follow the instructions there.

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Re: [time-nuts] 510 doubler

2015-01-28 Thread Gerhard Hoffmann

Am 28.01.2015 um 01:57 schrieb Charles Steinmetz:
(again, not many of us amateur time nuts).  Once upon a time, Motorola 
made monolithic quad BJTs -- but I'm not aware of any matched quads 
similar to 2Ns at this time.  [Several manufacturers still claim 
to make MPQs, but those are not monolithic and not matched.]



There still are
 http://www.analog.com/static/imported-files/data_sheets/MAT04.pdf 
 
http://www.intersil.com/content/dam/Intersil/documents/hfa3/hfa3046-3096-3127-3128.pdf 



if duals are enough:
 http://www.analog.com/static/imported-files/data_sheets/SSM2220.pdf ,
 http://www.analog.com/static/imported-files/data_sheets/MAT12.pdf 
also mat02, mat03, maybe SSM2110,


I have used most of them :-)
 
https://picasaweb.google.com/103357048842463945642/LowNoisePreamplifiers?authuser=0feat=directlink 




regards, Gerhard


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Re: [time-nuts] 510 doubler and old Toko RF catalogue (Cirkit 2nd ed.1994)

2015-01-27 Thread Alan Melia
Hi Andrea I have here a Cirkit  2nd edition Toko catalogue dated 1993 (a 
firm local to me I dealt with quite a lot) The cat is in good condition but 
it is 128 pages and a glued spine so scanning risks breaking it up. However 
the 10k range occupies just one page and if the part adjacent to the spine 
does not copy well all you will lose is the 100off price column (and I dont 
think you can buy them for that now 20 years on :-))  )  Give me a little 
time and I will do you a scan of the page, and mail it direct as a PDF.


I might actually have some new Toko coils in the component drawers but they 
may not be 10K. However I also have a lot of 5MHz OCXOs including Racal an 
Toyocom so I might have something useful if you dont find a source nearer to 
you.


Best Wishes
Alan
G3NYK

- Original Message - 
From: Andrea Baldoni erm1ea...@ermione.com

To: time-nuts@febo.com
Sent: Tuesday, January 27, 2015 3:53 PM
Subject: [time-nuts] 510 doubler and old Toko RF catalogue (Cirkit 2nd 
ed.1994)




Hello All.

Now I have some 5MHz DOCXO. I have started to experiment with them
and I would like to build a frequency doubler.
I already saw the very nice circuit from Gerhard Hoffmann for the Lucent, 
I saw

some diode circuits from Wenzel (my oscillators output around 1.5Vpp
loaded, too scarce for diodes alone; I used a 1:2 transformer just to try
and I obtained the 10MHz but not good for anything) and I saw the doubler
circuit Racal Dana used in some counters I attached.

I would like to build something like one of those; it's a full wave 
rectifier
made by a differential amplifier and two diodes, followed by a 10MHz 
amp/filter

chain much like the IF of FM radios (with AGC too!). I don't know if it's
adequate for serious use; I also saw the Z3811-80007 doubler board used in
Z3815A and Z3805A according to the seller, much more modern and surely 
better,

but I have not its schematic. Someone knows it?

I have bought one of the Racal units, just to have the opportunity to 
fiddle
with an already working one; I identified the IF transformers used there 
and
are Toko common 10.7MHz Q=80 unit. They are not built anymore but it's 
possible

to find similar ones in Internet; however it happens to me frequently
to need information about the old Toko 10K series and there is not any
comprehensive source. I saw I share this frustration with many people in 
the

electronics newsgroups.
Finally I found that a (fairly) complete Toko catalog existed, it was sold 
by

Cirkit in '94 and it's not available anymore.
Someone has it in PDF form, or want to borrow it to me to scan it?

By the way, I see that really many of the 10MHz reference out there, are 
in

effect doubled 5MHz ones so build a doubler seems reasonable for me.

Best regards,
Andrea Baldoni
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Re: [time-nuts] 510 doubler

2015-01-27 Thread Charles Steinmetz

Andrea wrote:


Now I have some 5MHz DOCXO. I have started to experiment with them
and I would like to build a frequency doubler.
 *   *   *
By the way, I see that really many of the 10MHz reference out there, are in
effect doubled 5MHz ones so build a doubler seems reasonable for me.


One thing to watch for is the 5MHz leakage component.  If you are 
going to use the 10MHz standard for time-nuts experiments, the 5MHz 
component needs to be WAY down ( -80dBc) or you will get funny 
periodic ripples in stability plots.  Despite having two 5MHz traps, 
one recently published design suppresses the 5MHz component only 
about 52dB below the 10MHz output, and the 20MHz and 30MHz components 
are also only -50 to -55dB.


For this reason (and some others, see discussions over the last 
several months in the archives) I prefer a doubler built with a 
quadrature hybrid coupler and a balanced mixer.  There is a write-up here:


http://www.ko4bb.com/manuals/download.php?file=02_GPS_Timing/4_App_Notes_and_Articles/Frequency_doubler_quadrature_DBM.pdf

I recently revived an old, stalled project to develop a JFET 
push-push doubler for use at 5MHz (see schematic below).


FETs with very high transconductance and very small pinchoff voltage 
(what a tube designer would call a sharp cutoff characteristic) 
(e.g., 2SK369, BF862, etc.) are attractive on first look because they 
can operate with lower conversion loss or even some conversion 
gain.  However, they are not well suited for doubler duty for two 
reasons: (i) their characteristics have a very short range of 
2nd-order curvature, so in order to keep noise down they must be 
driven into regions of higher-order distortion and therefore generate 
lots of spurious energy; and (ii) they are devilishly hard to match 
well enough to suppress the input frequency feedthrough.  Note that 
you also need to put enough voltage on the FET drains to get them 
well into the saturation region -- a Vcc of 5v is not enough.  Again, 
the penalty is lots of spurious energy.  So, the lower conversion 
loss of sharp-cutoff FETs is not the benefit it might at first appear 
to be -- it is much easier to add gain after the doubler than to 
remove unwanted spurious mixing products.


The design below uses medium-cutoff FETs and a Vcc of 15v (I found 
that J111 and J310 work best and can be matched sufficiently with a 
one-point match; 2N4416 and others also work, but are fussier and 
would benefit from a 2- or 3-point match).  At an input of 500mVrms, 
their long 2nd-order characteristic is used efficiently to generate 
10MHz with relatively little spurious energy.


I had no problem finding one or more FET pairs matched to within 1mV, 
given 20 devices from the same lot (YMMV).  With properly adjusted 
traps at 5, 20, and 30MHz, all spurious responses were below 
-80dBc.  The inductors can be commercial RF parts with Q of 200 or so 
(I used some high-quality through-hole RF inductors I had on hand -- 
I doubt any SMD inductors will work).  The trap capacitors should be 
C0G/NP0 ceramics for the bulk of the capacitance, plus very small 
trimmers (I used 27pF, 27pF, and 100pF plus 0.2--6pF glass piston 
trimmers).  I wound the two transformers on Mix-61 toroid cores (each 
winding is 20 turns on a FT37-61 core -- the inductance is a little 
lower than called out).  Mini-Circuits parts (or equivalents) may also work.


Best regards,

Charles

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Re: [time-nuts] 510 doubler

2015-01-27 Thread Bruce Griffiths
Using the square law characteristic will inevitably increase the phase noise 
floor particularly in the flicker region with respect to just using the 
switching characteristic of a JFET, diode or BJT  (non saturated).The only 
viable solution is to use better filtering of the output of a switching 
multiplier.If you intend to use a diode ring based mixer configuration diode 
connected (collector shorted to base) npns such as 2N222's are significantly 
quieter (as shown by NIST) than schottky diodes for frequencies below 40MHz or 
so.
Bruce. 

 On Wednesday, 28 January 2015 8:25 AM, Charles Steinmetz 
csteinm...@yandex.com wrote:
   

 Andrea wrote:

Now I have some 5MHz DOCXO. I have started to experiment with them
and I would like to build a frequency doubler.
      *  *  *
By the way, I see that really many of the 10MHz reference out there, are in
effect doubled 5MHz ones so build a doubler seems reasonable for me.

One thing to watch for is the 5MHz leakage component.  If you are 
going to use the 10MHz standard for time-nuts experiments, the 5MHz 
component needs to be WAY down ( -80dBc) or you will get funny 
periodic ripples in stability plots.  Despite having two 5MHz traps, 
one recently published design suppresses the 5MHz component only 
about 52dB below the 10MHz output, and the 20MHz and 30MHz components 
are also only -50 to -55dB.

For this reason (and some others, see discussions over the last 
several months in the archives) I prefer a doubler built with a 
quadrature hybrid coupler and a balanced mixer.  There is a write-up here:

http://www.ko4bb.com/manuals/download.php?file=02_GPS_Timing/4_App_Notes_and_Articles/Frequency_doubler_quadrature_DBM.pdf

I recently revived an old, stalled project to develop a JFET 
push-push doubler for use at 5MHz (see schematic below).

FETs with very high transconductance and very small pinchoff voltage 
(what a tube designer would call a sharp cutoff characteristic) 
(e.g., 2SK369, BF862, etc.) are attractive on first look because they 
can operate with lower conversion loss or even some conversion 
gain.  However, they are not well suited for doubler duty for two 
reasons: (i) their characteristics have a very short range of 
2nd-order curvature, so in order to keep noise down they must be 
driven into regions of higher-order distortion and therefore generate 
lots of spurious energy; and (ii) they are devilishly hard to match 
well enough to suppress the input frequency feedthrough.  Note that 
you also need to put enough voltage on the FET drains to get them 
well into the saturation region -- a Vcc of 5v is not enough.  Again, 
the penalty is lots of spurious energy.  So, the lower conversion 
loss of sharp-cutoff FETs is not the benefit it might at first appear 
to be -- it is much easier to add gain after the doubler than to 
remove unwanted spurious mixing products.

The design below uses medium-cutoff FETs and a Vcc of 15v (I found 
that J111 and J310 work best and can be matched sufficiently with a 
one-point match; 2N4416 and others also work, but are fussier and 
would benefit from a 2- or 3-point match).  At an input of 500mVrms, 
their long 2nd-order characteristic is used efficiently to generate 
10MHz with relatively little spurious energy.

I had no problem finding one or more FET pairs matched to within 1mV, 
given 20 devices from the same lot (YMMV).  With properly adjusted 
traps at 5, 20, and 30MHz, all spurious responses were below 
-80dBc.  The inductors can be commercial RF parts with Q of 200 or so 
(I used some high-quality through-hole RF inductors I had on hand -- 
I doubt any SMD inductors will work).  The trap capacitors should be 
C0G/NP0 ceramics for the bulk of the capacitance, plus very small 
trimmers (I used 27pF, 27pF, and 100pF plus 0.2--6pF glass piston 
trimmers).  I wound the two transformers on Mix-61 toroid cores (each 
winding is 20 turns on a FT37-61 core -- the inductance is a little 
lower than called out).  Mini-Circuits parts (or equivalents) may also work.

Best regards,

Charles


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[time-nuts] 510 doubler and old Toko RF catalogue (Cirkit 2nd ed. 1994)

2015-01-27 Thread Andrea Baldoni
Hello All.

Now I have some 5MHz DOCXO. I have started to experiment with them
and I would like to build a frequency doubler.
I already saw the very nice circuit from Gerhard Hoffmann for the Lucent, I saw
some diode circuits from Wenzel (my oscillators output around 1.5Vpp
loaded, too scarce for diodes alone; I used a 1:2 transformer just to try
and I obtained the 10MHz but not good for anything) and I saw the doubler
circuit Racal Dana used in some counters I attached.

I would like to build something like one of those; it's a full wave rectifier
made by a differential amplifier and two diodes, followed by a 10MHz amp/filter
chain much like the IF of FM radios (with AGC too!). I don't know if it's
adequate for serious use; I also saw the Z3811-80007 doubler board used in
Z3815A and Z3805A according to the seller, much more modern and surely better,
but I have not its schematic. Someone knows it?

I have bought one of the Racal units, just to have the opportunity to fiddle
with an already working one; I identified the IF transformers used there and
are Toko common 10.7MHz Q=80 unit. They are not built anymore but it's possible
to find similar ones in Internet; however it happens to me frequently
to need information about the old Toko 10K series and there is not any
comprehensive source. I saw I share this frustration with many people in the
electronics newsgroups.
Finally I found that a (fairly) complete Toko catalog existed, it was sold by
Cirkit in '94 and it's not available anymore.
Someone has it in PDF form, or want to borrow it to me to scan it?

By the way, I see that really many of the 10MHz reference out there, are in
effect doubled 5MHz ones so build a doubler seems reasonable for me.

Best regards,
Andrea Baldoni
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