So, I thought I would sweep the frustum BEFORE soldering closed...yeah I know, its not a good idea. So, looks like center is around 2.474 GHz, higher than the model, but within mag range. Return Loss 43dB which is outstanding without solder. If I measure Q from 3dB off best RL, it would be crazy high. Not going to go there yet, things will change after it gets soldered. Bottom line, almost ready to button up...
You folks are all re-inventing resonant cavity filters. A return loss of 43 db is OK, but not great, and the Q should be well over 100,000 for a good design, even with a basic plated aluminum cavity. Again, once more. You can design a filter for an expected signal, or you can TUNE THE SOURCE for an expected Q. You folks seems to be slowly re-learning basic microwave engineering, and I'm glad to see that there is more talk of making the source track resonance, rather than trying to micro-machine a cavity to resonate with a crap source like a magnetron.
EW references to 20 Newtons per Kilowatt give me hope, but I'm not holding my breath because I don't want to turn blue.
EDIT: The s-parameter measurements you all make are only as good as the source and receiver you have on hand. Cheap USB instruments are severly limited in performance (simple physics). Phase noise, AM/PM conversion, lack of phase information ALL contribute to lack of useful information. Again, s-parameters are impedance specific, by definition. If the system is not normalized to a particular (generally 50 ohm) impedance, the results are useless. I have seen NO attempt by ANYONE on this forum to normalize their impedance. Any reference to injected power levels, or S-Parameters, are therefore worthless.
Note: A magnetron is most definitely NOT a 50 ohm source, nor is a microwave oven a 50 ohm load. The take away is that an Em drive cavity is not a 50 ohm load, and should never be modeled as such.
Shell, if you're still on...re this image of yours, I don't recall exactly; this very clean frequency/signal was the result of powering your Maggie with DC, but is it fair to assume that it is a water cooled Maggie and you experience no "signal drift" related to the active cooling ? thnx FL
Before my amp died some of the tests I did indicated the best thrust freq was not the same as the best rtn loss freq. I believe this is due to frustum manufacturing errors introducing phase distortion in the multiple reflected travelling waves being compensated by a slightly off freq exciton such that the say negative phase distortions introduced by the freq are compensated by positive phase distortions caused by the manufacturing defects resulting in the min overall phase distortions over the life of the travelling wave & thus generating a higher thrust than operating at best rtn loss freq.
I also found the thrust bandwidth was very much narrower than the rtn loss bandwidth.
This info is preliminary & needs to be confirmed by a lot more tests when I get my amp back.Quote...Agreed on both counts.
I’ve seen the same thing, (max force freq. not equal to min VSWR freq, and peak force output having a narrower BW than the RF resonant cavity’s -3dB bandwidth)...
Shell, if you're still on...re this image of yours, I don't recall exactly; this very clean frequency/signal was the result of powering your Maggie with DC, but is it fair to assume that it is a water cooled Maggie and you experience no "signal drift" related to the active cooling ? thnx FLThe critical things you need to do for the magnetron to clean up the output. Don't forget magnetrons are used in the semiconductor industry and need to have a clean output and a stable output.
Clean DC to the magnetron. Critical as it keeps the splattering and AM and also any DC component and removes the 50% chopped duty cycles from regular microwave power supplies.
Thermal cooling other than air. Coiled copper water cooling through a heat exchanger works well. Need more cooling then submerse in chilled water.
Turn off the magnetron heater after 3-4 seconds, you don't need it after.
Shell
So, I thought I would sweep the frustum BEFORE soldering closed...yeah I know, its not a good idea. So, looks like center is around 2.474 GHz, higher than the model, but within mag range. Return Loss 43dB which is outstanding without solder. If I measure Q from 3dB off best RL, it would be crazy high. Not going to go there yet, things will change after it gets soldered. Bottom line, almost ready to button up...
You folks are all re-inventing resonant cavity filters. A return loss of 43 db is OK, but not great, and the Q should be well over 100,000 for a good design, even with a basic plated aluminum cavity. Again, once more. You can design a filter for an expected signal, or you can TUNE THE SOURCE for an expected Q. You folks seems to be slowly re-learning basic microwave engineering, and I'm glad to see that there is more talk of making the source track resonance, rather than trying to micro-machine a cavity to resonate with a crap source like a magnetron.
EW references to 20 Newtons per Kilowatt give me hope, but I'm not holding my breath because I don't want to turn blue.
EDIT: The s-parameter measurements you all make are only as good as the source and receiver you have on hand. Cheap USB instruments are severly limited in performance (simple physics). Phase noise, AM/PM conversion, lack of phase information ALL contribute to lack of useful information. Again, s-parameters are impedance specific, by definition. If the system is not normalized to a particular (generally 50 ohm) impedance, the results are useless. I have seen NO attempt by ANYONE on this forum to normalize their impedance. Any reference to injected power levels, or S-Parameters, are therefore worthless.
Note: A magnetron is most definitely NOT a 50 ohm source, nor is a microwave oven a 50 ohm load. The take away is that an Em drive cavity is not a 50 ohm load, and should never be modeled as such.
So, I thought I would sweep the frustum BEFORE soldering closed...yeah I know, its not a good idea. So, looks like center is around 2.474 GHz, higher than the model, but within mag range. Return Loss 43dB which is outstanding without solder. If I measure Q from 3dB off best RL, it would be crazy high. Not going to go there yet, things will change after it gets soldered. Bottom line, almost ready to button up...
You folks are all re-inventing resonant cavity filters. A return loss of 43 db is OK, but not great, and the Q should be well over 100,000 for a good design, even with a basic plated aluminum cavity. Again, once more. You can design a filter for an expected signal, or you can TUNE THE SOURCE for an expected Q. You folks seems to be slowly re-learning basic microwave engineering, and I'm glad to see that there is more talk of making the source track resonance, rather than trying to micro-machine a cavity to resonate with a crap source like a magnetron.
EW references to 20 Newtons per Kilowatt give me hope, but I'm not holding my breath because I don't want to turn blue.
EDIT: The s-parameter measurements you all make are only as good as the source and receiver you have on hand. Cheap USB instruments are severly limited in performance (simple physics). Phase noise, AM/PM conversion, lack of phase information ALL contribute to lack of useful information. Again, s-parameters are impedance specific, by definition. If the system is not normalized to a particular (generally 50 ohm) impedance, the results are useless. I have seen NO attempt by ANYONE on this forum to normalize their impedance. Any reference to injected power levels, or S-Parameters, are therefore worthless.
Note: A magnetron is most definitely NOT a 50 ohm source, nor is a microwave oven a 50 ohm load. The take away is that an Em drive cavity is not a 50 ohm load, and should never be modeled as such.
... Use a tuner and calibrate the system before {open(r=+1_j0),load(50R),short(r=-1_j0)}
I know calibration kits are expensive but it works, uncalibrated your VNA is less helpful.
https://www.maurymw.com/Precision/VNA_Cal_Kits.php
...
don't know if your USB-series-VNA have a cal mode (it has to have i think)
OK this was a tip for people using a noisy magnetron as source because its cheap but not tunable in frequency.
Its less of interest what is tuned, the source frequency at fixed resonator geometry or the cavity at fixed frequency of the source(movable endplate or similar). If this done well the result is similar.
But again I am with you, If a tunable source(+amp) is available (maybe PLL control) it is much easier to tune the frequency.
BTW there are automated mechanical stub tuners available at the market.
http://www.mksinst.com/docs/UR/SmartMatch-DS.pdf
A mechanical cavity tuning could be automated in the same way.
ReplyQuoteNotify...
Quote...A mechanical cavity tuning could be automated in the same way.
Interesting new comment from Dr. Mike McCulloch on his EmDrive theory:
https://twitter.com/memcculloch/status/731774299380568064?s=01
Both Mike & Roger talk about the thrust being produced by larger EmWave momentum / mass at the big end and smaller EmWave monentum / mass at the small end with the EmDrive thrust being the result of gained momentum from the lost EmWave momentum / mass differential between the big & small ends.
http://physicsfromtheedge.blogspot.com/2015/06/crit-of-shawyers-emdrive-theory.htmlI was about to post how I assumed that the "higher inertial mass" near the large end in Dr. McCulloch's theory must be meant in a way that the total momentum in the photons is reduced when the mass increases.* This post from him confirms he understands the direction issue with Shawyer's theory, so he isn't likely to be making the same mistake, and comparisons of his McCulloch's increased mass to Shawyer's increased momentum are wrong.
* I don't understand how inertial mass even makes sense when talking about photons, but McCulloch's theory has room with new physics, general relativity, and interactions between photons and other radiation that can presumably carry momentum away from the cavity. My limited understanding is that the increase in mass comes with transfer of momentum to Unruh waves, so that the momentum decreases despite the increase in mass. I could be off base, and there are other consistent interpretations I can think of.
In general relativity, gravity affects anything with momentum and energy. Photons do not have a rest-mass, but they do have momentum, and energy--and they are thus effected by gravity (photons cannot leave a black hole and their path in space is affected by the geodesics imposed by a massive object like the Sun).
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So far I believed, that having standing waves inside the cavity of any shape implies, these waves have everywhere the very same wavelength. First of all we should demonstrate, that the wavelength of standing waves changes inside the conical resonator along its axis - if it doesn't change, then no dependence of photon mass on wavelength applies and the whole above line of reasoning is wrong with massive photons or without them (not to say, it would be also redundant with respect to the "Unruh radiation" stuff anyway).




So, I thought I would sweep the frustum BEFORE soldering closed...
Yes, the usb vna has the open, short and load cal kit. The OP is mistaken about 43dB rl. Try to buy a 900W load or cavity and post the rl specs. Better yet, they can build an assymetric cavity themselves and prove their statement.
In an EM Drive, the wavelength is smaller towards the big end and the wavelength gets bigger towards the small end:
In an EM Drive, the wavelength is smaller towards the big end and the wavelength gets bigger towards the small end:
Maybe review the attached as Roger shows how his EmDrive cavity generates a momentum gradient that transfers lost small end momentum (big end - small end momentum) to the cavity such that big end momentum = small end momentum + cavity gained momentum to balance overall momentum.
So it seems Mike & Roger are different dogs but with the same leg action.
...
Maybe review the attached.
Yes, the usb vna has the open, short and load cal kit. The OP is mistaken about 43dB rl. Try to buy a 900W load or cavity and post the rl specs. Better yet, they can build an assymetric cavity themselves and prove their statement.
Conical frustrums have an infinite number of planes that divide the shape into two symmetric halves.Its a strange beast I've never seen the likes of before. Its almost as if you take a great cavity and distort its natural resonance modes. This bifurcation is certainly something new to me. Shawyer picked up on it and as Rodal says, he might not have the correct theory, but others like White and McCullough are theorizing this new form factor produces an unexpected result. Still quite interesting that CoM might be responsible for the momentum and therefore it's prohibiting a violation. Will this classical physics law be the key to the observed effect? Don't know but this is the kind of stuff that "fascinates" me.
Actually, I think what were doing here is creating a single frequency RF load by using a cavity filter...weird.
So, I thought I would sweep the frustum BEFORE soldering closed...
What are you using for a signal generator? I got official approval from the spouse to purchase the USB spectrum analyser, so now i'm looking for an economical signal generator.
Also, how do you like VNA/J?The VNA/J is great...no sig gen needed. Its normalized just like the old school benchtop units I used to tweek endlessly. Granted you won't get the absolute accuracy, but several hundred $ versus several thousands make it a no-brainer. Tuning cavity filters are best done with sig gens with calibrated cables and connectors, but there again, several thousands for a lab quality generator not to mention the cal kits and cables. Slow the sweep rate down and narrow the display BW on the VNA/J and you'll do just fine I believe.
(No internet). Even cyl cavity has var wavelength in grav field or accl frame of reference