Did you use one-ply, two-ply, or three-ply TP?
More seriously, your LTE-Lite differs in a couple of respects from the
batch of "production" ones, or at least my example. Your TCXO seems to be
in a metal package (shiny gold colour) and open to the air, if I'm
interpreting the photo on your LTE-Lite page correctly (and also the photo
that Said posted in his divide-by-two document). The production units have
the TCXO in a solid black package, probably black epoxy, with a blob of RTV
rubber on top. So the "production" units are probably already somewhat
better shielded against drafts.
(Thanks for doing the tests, particularly for those of us who can't do
these tests ourselves. I can only watch the 1 PPS of the LTE-Lite wander
with respect to the 1 PPS from my old Thunderbolt (Piezo oscillator), and
look at the worst-case variation, but I have no way of knowing how much of
the drift is due to each GPSDO).
On Sun, Nov 23, 2014 at 11:24 AM, Tom Van Baak tvb@leapsecond.com wrote:
The short-term performance is 10x worse if you don't shield the TCXO from
air, even if the ambient air is "still". I suggested Said sell the product
with some sort of engineered shield in place. Instead each of us will solve
the problem in our own way; which is ok for a dev kit.
For plots and photos showing performance with, and without, and with
insulation see:
http://leapsecond.com/pages/LTE-Lite/
The difference is dramatic, especially if you are used to working with
OCXO where this sort of effect does not occur.
The insulation may be found in convenient rolls at many local stores. I
used TP, which for this application is an acronym for Thermal Paper.
/tvb
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On 23 Nov 2014 16:25, "Tom Van Baak" tvb@leapsecond.com wrote:
For plots and photos showing performance with, and without, and with
insulation see:
http://leapsecond.com/pages/LTE-Lite/
The difference is dramatic, especially if you are used to working with
OCXO where this sort of effect does not occur.
Tom,
What plots are with and without the thermal paper?
I see several graphs, but don't know what is under what conditions.
The second graph shows something fairly significant happening at 300 s. Is
that where you removed the TP?
Dave
Hi
Well the answer is obvious:)
You simply need to turn on the air-conditioning full blast for more months of the summer in … ummm ….. errrr …. Denmark … hmmm…..
Heat only or cool only systems seem to be more practical when the heat sink is a flowing body of water or an ocean. Unfortunately those seem to also run up the price of adjacent real estate.
Moving bodies of water also aren’t very good for stabilizing temperature on a frequency source. The same thing is true of a hole in the ground that goes above or below the level of ground water over the course of the year. If you drill a hole, there is indeed a wrong depth to pick. It might be interesting to see how deep you need to go for stable ground water temps. Around here the top layer of ground water was rain last week or last month.
Bob
On Nov 23, 2014, at 1:07 PM, Poul-Henning Kamp phk@phk.freebsd.dk wrote:
In message CANX10hCaoB-5GYsbR7sdXwL7DYH7QUBMhXWmi9xDRcF3mDM7_Q@mail.gmail.com
, "Dr. David Kirkby (Kirkby Microwave Ltd)" writes:
Geothermal means you drill at least 50m (Iceland) or more likely
half a kilometer down, in order to harvest water at near boiling
point from the Earths geological heat-sources (mostly uranium decay).
Sorry. What he installs is pipes in the ground in residential or
industrial sites. Basically he says they work initially, but performance
drops dramatically over a couple of years.
That is not "geothermal" then, and yes, a LOT of those systems are
badly underdimensioned.
I've been researching this topic intensively because my new house
will be heated that way.
My conclusion, based on reading a lot of reports, is that there
is no credible way to predict the performance. The wetter your
soil the better, but that's about it.
I'm going to overprovision by a factor two to be on the safe side,
afterall it only costs EUR7 for each extra meter of pipe.
--
Poul-Henning Kamp | UNIX since Zilog Zeus 3.20
phk@FreeBSD.ORG | TCP/IP since RFC 956
FreeBSD committer | BSD since 4.3-tahoe
Never attribute to malice what can adequately be explained by incompetence.
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Hi
There are two plots with activity changing at 300 seconds. The second plot (purple) is the removal of the paper at 300 seconds. The fourth plot (red) is the addition of the paper at 300 seconds.
The last plot (green and blue) is ADEV with and without the paper. Blue is ADEV with paper. Green is ADEV without paper.
The second to last plot demonstrates the unit meeting 1x10^-9 (peak to peak) frequency stability with the paper over a 1,000 second test. It shows it doing about 5X worse on frequency stability over the same period without the paper. Yes, that’s all with 1 second averaging. Changing the averaging would impact each of the results. It should change their ratio.
Again back to the basic question: frequency over what period? Go to a 24 hour average and the results should be terrific. In some systems, that’s a useful number (I guess….). I rarely see people set their counters to an 86,000 second gate time :)
Bob
On Nov 23, 2014, at 4:42 PM, Dr. David Kirkby (Kirkby Microwave Ltd) drkirkby@kirkbymicrowave.co.uk wrote:
On 23 Nov 2014 16:25, "Tom Van Baak" tvb@leapsecond.com wrote:
For plots and photos showing performance with, and without, and with
insulation see:
http://leapsecond.com/pages/LTE-Lite/
The difference is dramatic, especially if you are used to working with
OCXO where this sort of effect does not occur.
Tom,
What plots are with and without the thermal paper?
I see several graphs, but don't know what is under what conditions.
The second graph shows something fairly significant happening at 300 s. Is
that where you removed the TP?
Dave
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Tom,
From the looks of the plots these may be from the first proto unit with early software no? Also was this with the indoor GPS antenna setup?
The production units with outdoor or windowed' antenna should have significantly improved average performance from the first unit and its early GPS and GPSDO firmware versions.
Bye,
Said
Sent From iPhone
On Nov 23, 2014, at 14:18, Bob Camp kb8tq@n1k.org wrote:
Hi
There are two plots with activity changing at 300 seconds. The second plot (purple) is the removal of the paper at 300 seconds. The fourth plot (red) is the addition of the paper at 300 seconds.
The last plot (green and blue) is ADEV with and without the paper. Blue is ADEV with paper. Green is ADEV without paper.
The second to last plot demonstrates the unit meeting 1x10^-9 (peak to peak) frequency stability with the paper over a 1,000 second test. It shows it doing about 5X worse on frequency stability over the same period without the paper. Yes, that’s all with 1 second averaging. Changing the averaging would impact each of the results. It should change their ratio.
Again back to the basic question: frequency over what period? Go to a 24 hour average and the results should be terrific. In some systems, that’s a useful number (I guess….). I rarely see people set their counters to an 86,000 second gate time :)
Bob
On Nov 23, 2014, at 4:42 PM, Dr. David Kirkby (Kirkby Microwave Ltd) drkirkby@kirkbymicrowave.co.uk wrote:
On 23 Nov 2014 16:25, "Tom Van Baak" tvb@leapsecond.com wrote:
For plots and photos showing performance with, and without, and with
insulation see:
http://leapsecond.com/pages/LTE-Lite/
The difference is dramatic, especially if you are used to working with
OCXO where this sort of effect does not occur.
Tom,
What plots are with and without the thermal paper?
I see several graphs, but don't know what is under what conditions.
The second graph shows something fairly significant happening at 300 s. Is
that where you removed the TP?
Dave
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Hi
A lot of these parts are designed for use in a system environment rather than sitting out on a bench. That’s as true of the KS boxes (forced air cooling) as it is of the LTE’s. In > 90% (and likely > 99.9%) of the places a TCXO gets used, it’s packed tight in with a bunch of other stuff. Not only is there no air movement, there might not be much air. A cell phone is a good example of this sort of assembly. Other battery powered portable gear fit this same general model, but possibly not to the same degree of “cram it in".
Yes, we love our big rack mounted boxes full of this or that. They are useful. The TCXO guys would go broke quickly if that was the market they focused their main efforts on. Big Morion 2” x 2” x 1” OCXO’s, yes those are targeted more at big rack mount this or that. Different market focus for different products. It’s not a one size fits all world.
Indeed, adapting a TCXO to a bench environment is something that you need to do. A nice fluffy cotton towel works quite well. Yes, that’s a 1970’s solution to the problem. Most TCXO’s were bigger back then. The issue has been around “for a while”. It’s actually not a bad thing to keep handy when testing OCXO’s. If they don’t work you can always use it to cry into …:)
Bob
On Nov 23, 2014, at 11:24 AM, Tom Van Baak tvb@LeapSecond.com wrote:
The short-term performance is 10x worse if you don't shield the TCXO from air, even if the ambient air is "still". I suggested Said sell the product with some sort of engineered shield in place. Instead each of us will solve the problem in our own way; which is ok for a dev kit.
For plots and photos showing performance with, and without, and with insulation see:
http://leapsecond.com/pages/LTE-Lite/
The difference is dramatic, especially if you are used to working with OCXO where this sort of effect does not occur.
The insulation may be found in convenient rolls at many local stores. I used TP, which for this application is an acronym for Thermal Paper.
/tvb
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Hi
Actually that was Bob trying to explain Tom’s plots simply from looking at them. I think I got it right, but it’s Tom’s data and his LTE part. Others have commented that Tom’s part looks different than theirs.
Maybe Tom needs a Microsoft Windows Update on his GPSDO firmware :) For some reason the very thought of Microsoft getting involved in something like that makes me shudder…
Bob
On Nov 23, 2014, at 5:33 PM, Said Jackson via time-nuts time-nuts@febo.com wrote:
Tom,
From the looks of the plots these may be from the first proto unit with early software no? Also was this with the indoor GPS antenna setup?
The production units with outdoor or windowed' antenna should have significantly improved average performance from the first unit and its early GPS and GPSDO firmware versions.
Bye,
Said
Sent From iPhone
On Nov 23, 2014, at 14:18, Bob Camp kb8tq@n1k.org wrote:
Hi
There are two plots with activity changing at 300 seconds. The second plot (purple) is the removal of the paper at 300 seconds. The fourth plot (red) is the addition of the paper at 300 seconds.
The last plot (green and blue) is ADEV with and without the paper. Blue is ADEV with paper. Green is ADEV without paper.
The second to last plot demonstrates the unit meeting 1x10^-9 (peak to peak) frequency stability with the paper over a 1,000 second test. It shows it doing about 5X worse on frequency stability over the same period without the paper. Yes, that’s all with 1 second averaging. Changing the averaging would impact each of the results. It should change their ratio.
Again back to the basic question: frequency over what period? Go to a 24 hour average and the results should be terrific. In some systems, that’s a useful number (I guess….). I rarely see people set their counters to an 86,000 second gate time :)
Bob
On Nov 23, 2014, at 4:42 PM, Dr. David Kirkby (Kirkby Microwave Ltd) drkirkby@kirkbymicrowave.co.uk wrote:
On 23 Nov 2014 16:25, "Tom Van Baak" tvb@leapsecond.com wrote:
For plots and photos showing performance with, and without, and with
insulation see:
http://leapsecond.com/pages/LTE-Lite/
The difference is dramatic, especially if you are used to working with
OCXO where this sort of effect does not occur.
Tom,
What plots are with and without the thermal paper?
I see several graphs, but don't know what is under what conditions.
The second graph shows something fairly significant happening at 300 s. Is
that where you removed the TP?
Dave
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On 11/23/14, 11:15 AM, Alex Pummer wrote:
by us in central California, we get 1kW/h square meter average around
the year, the south even more, el Cajon will have today +29C° in the
afternoon as of 23 of November 2014
I suspect more like the insolation peaks at 1kW/square meter or a bit
more, the average over a day is somewhat less. At JPL we have a weather
station on line that displays this and I don't recall seeing
significantly more than 1000 W/m2.
The nominal average 1.362 kW/sq meter at solar max is at the top of the
atmosphere, and is normal to the incidence.
The surface insolation at the equator when the sun is directly overhead
is about 1.04 kW/sq meter.
I think you'd get pretty close to that at solar noon in the Summer in
Southern California, which is 32-34 degrees latitude, so at the
solstice, the zenith angle is 10 degrees, and cos(10) is pretty close to 1.
You do pick up some additional insolation from diffuse and scattered
radiation from clouds or haze, but I'm not sure that makes up for the
attenuation due to the same haze.
Some time ago, I calculated that in Los Angeles (34 degrees latitude), a
horizontal flat plate gets about 8-9 kWh/m2/day in summer and about 1-2
kWh/m2/day in winter.. Tilting the collector would help a lot in the
winter (Zenith angle is 56 degrees instead of 10), but there's no making
up for the short days.
Getting back to the time-nuts aspects, there are some charts around that
show the temperature variation as a function of depth, latitude, soil
and season. I know that for DSN, they went through all kinds of
gyrations to calculate (and measure) this for the optical fiber timing
links between the antennas and the masers. For small dissipated power
(I doubt your oscillator is going to be putting kilowatts into the soil)
you don't have to go very deep (single digit meters) before the diurnal
variation is down in the 0.1 degree or smaller. Annual variations are
bigger.
http://www.builditsolar.com/Projects/Cooling/EarthTemperatures.htm
has a bunch of charts for some unknown latitude (probably mid Atlantic
states, since the data is from Virginia Tech). They appear to use well
water temperatures as the measurement technique.
A bit more googling found a paper by one G. Florides that refers to the
Kasuda formula.. (the link is hard to cut and paste.. I'm sure if you
google "Florides soil temperature" you'll find it)
and gives this reference
Kasuda, T., and Archenbach, P.R. "Earth Temperature and Thermal
Diffusivity at Selected Stations in the United States", ASHRAE
Transactions, Vol. 71, Part 1, 1965.
Horizontal ground heat means that you are harvesting sunshine
accumulated in the top one meter of the soil. Much of the energy
is harvested from freezing the water around the pipe thus pulling
out the relatively high melting energy of water.
A Hint about avoiding convective cell heat transfer,
If you keep the spacing between two planes less than 5/16" then you will
be unlikely to have convection cells forming. The stationary air is a good insulator
but thermal radiation will be the dominant heat transfer process.
This is true for double glazing, katharometers and generally all devices.
The suppression of turbulent heat transfer may provide more insulation but also
less noise and instability.
So it may be a good idea to use a relatively close fitting box with thick walls.
Cheers,
Neville Michie
On 23/11/2014, at 11:37 PM, Charles Steinmetz wrote:
Dave wrote
But given the TCXO"s sensitivity to temperature changes, I don't
know whether it might be preferable to mount the LTE lite in its own box
without any power supplies in it - perhaps with some thermally insulting
material around the LTE lite so the crystal doesn't experience any fast
temperature changes.
First, mount the LTE in a cast aluminum box (not thin sheet metal, something with some heft). Use thermally insulating standoffs (teflon or nylon, with no metal "through" fasteners) to get the board in the middle of the volume of the box. Use a box a bit larger than you'd first think, so there is at least 1" of air on all 6 sides of the LTE board. Do NOT mount any part of the LTE board (connectors, etc.) directly to the box walls -- use "pigtails" for all connections. Do NOT use any insulation between the LTE and the box walls other than the 1"+ of air.
The mounting described above will add substantial thermal capacitance to the LTE board (good) without adding significant thermal resistance (bad). For further discussions of this issue, search the list archives for "thermal capacitance" and "thermal mass."
Now, mount the cast box (plus any thermal mass you add to it -- see below) so that IT is thermally isolated from the overall enclosure (or, if it sits out in the open, thermally isolated from anything solid). The air space in the enclosure isolates the oscillator from the cast box and the box is sufficiently massive that its temperature cannot change nearly as fast as ambient. The thermal mass of the cast box can be adjusted by adding thermal mass to it as desired.
The goal is for the box temperature to change only by changes in ambient AIR temperature, and the LTE board to change only by changes in the AIR temperature inside the cast box. This integrates any changes to the LTE board temperature with a very long time constant, which allows the GPS discipline to track and cancel the temperature changes.
(If you mount an ovenized oscillator this same way, it integrates any changes to the OCXO temperature so that the oven control loop can track and cancel any changes to the crystal temperature.)
You can, of course, improve things even further by making sure the ambient air temperature surrounding the cast box changes slowly, or not at all. But the technique described above can be counted on to reduce thermal effects in most OCXOs or GPSDOs to better (often much better) than the 1e-13 level unless the ambient temperature changes MUCH more and MUCH faster than any change we wouild consider normal for a living space. This is true whether the cast box is mounted out in the open, or inside an overall enclosure with other electronics.
Best regards,
Charles
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Hi
I believe that if you go back a few years in the archives, you will find a thread that ultimately stops with a swimming pool full of mercury. Needless to say, we’re been down this road once or twice before.
Bob
On Nov 23, 2014, at 7:59 PM, Neville Michie namichie@gmail.com wrote:
A Hint about avoiding convective cell heat transfer,
If you keep the spacing between two planes less than 5/16" then you will
be unlikely to have convection cells forming. The stationary air is a good insulator
but thermal radiation will be the dominant heat transfer process.
This is true for double glazing, katharometers and generally all devices.
The suppression of turbulent heat transfer may provide more insulation but also
less noise and instability.
So it may be a good idea to use a relatively close fitting box with thick walls.
Cheers,
Neville Michie
On 23/11/2014, at 11:37 PM, Charles Steinmetz wrote:
Dave wrote
But given the TCXO"s sensitivity to temperature changes, I don't
know whether it might be preferable to mount the LTE lite in its own box
without any power supplies in it - perhaps with some thermally insulting
material around the LTE lite so the crystal doesn't experience any fast
temperature changes.
First, mount the LTE in a cast aluminum box (not thin sheet metal, something with some heft). Use thermally insulating standoffs (teflon or nylon, with no metal "through" fasteners) to get the board in the middle of the volume of the box. Use a box a bit larger than you'd first think, so there is at least 1" of air on all 6 sides of the LTE board. Do NOT mount any part of the LTE board (connectors, etc.) directly to the box walls -- use "pigtails" for all connections. Do NOT use any insulation between the LTE and the box walls other than the 1"+ of air.
The mounting described above will add substantial thermal capacitance to the LTE board (good) without adding significant thermal resistance (bad). For further discussions of this issue, search the list archives for "thermal capacitance" and "thermal mass."
Now, mount the cast box (plus any thermal mass you add to it -- see below) so that IT is thermally isolated from the overall enclosure (or, if it sits out in the open, thermally isolated from anything solid). The air space in the enclosure isolates the oscillator from the cast box and the box is sufficiently massive that its temperature cannot change nearly as fast as ambient. The thermal mass of the cast box can be adjusted by adding thermal mass to it as desired.
The goal is for the box temperature to change only by changes in ambient AIR temperature, and the LTE board to change only by changes in the AIR temperature inside the cast box. This integrates any changes to the LTE board temperature with a very long time constant, which allows the GPS discipline to track and cancel the temperature changes.
(If you mount an ovenized oscillator this same way, it integrates any changes to the OCXO temperature so that the oven control loop can track and cancel any changes to the crystal temperature.)
You can, of course, improve things even further by making sure the ambient air temperature surrounding the cast box changes slowly, or not at all. But the technique described above can be counted on to reduce thermal effects in most OCXOs or GPSDOs to better (often much better) than the 1e-13 level unless the ambient temperature changes MUCH more and MUCH faster than any change we wouild consider normal for a living space. This is true whether the cast box is mounted out in the open, or inside an overall enclosure with other electronics.
Best regards,
Charles
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