Wait...if you are deciding either/or, get youself the miniVNA tiny/VNA/J and not the sig gen. You will need a spec an though.
Wait...if you are deciding either/or, get youself the miniVNA tiny/VNA/J and not the sig gen. You will need a spec an though.
So the $330 RF Instruments SA0314 spectrum analyser + the $560 miniVNA tiny + the free VNA/J = ~$900That's the route I took, yes.
If this works out, Shawyer may prove to have had the right stuff "inventor's intuition". What I don't understand is why Shawyer dismisses other explanations like McCulloch's, White's etc: Edison, Westinghouse and Tesla didn't debate theories with Hertz: they invented and experimented.
Even Dr. White did not discuss his theory in his 2004 AIAA paper, which concentrated on the experiments.
Hi all
I guess by now you have all measured thrust from your experimental EmDrives. The measured results are likely to vary considerably with stability of input match, the type of measurement system etc. However it is likely that your experiments can enable verification of some aspects of the classic theory of EmDrive operation to be tested. This work has been carried out in a number of research organisations, and in each case the predictions of classic theory have been demonstrated.
I have taken the liberty of attaching a presentation of basic theory. This is a “high level” presentation aimed at non-specialists but it summarises the results of many years of discussion, argument and study amongst professional Physicists, Mathematicians and Engineers on both sides of the Atlantic.
In particular two aspects can be noted.
Inside the cavity Einstein rules, EM waves travel at relativistic velocities and the EmDrive can be considered an open system. This was first pointed out many years ago by an eminent UK government scientist working at Farnborough, the late David Fearn. If the cavity is operated below cut-off frequency, travelling waves are distorted and thrust approaches zero.
Outside the cavity Newton rules, thus action and reaction are equal and opposite. A fully constrained EmDrive thruster will therefore not exhibit thrust, whilst an unconstrained thruster will accelerate in the opposite direction to the thrust vector. Any static thrust measurement system will apply some constraint to the thruster and depending on spring constants etc, it can be set up to measure thrust, reaction force or zero force.
Unfortunately I am not now able to enter into public disclosure of anything other than general theory and the experimental work already published, but the information in the attachment has been widely discussed and feel free to distribute it and discuss it as you wish.
Good luck with your work, I hope that successful public experiments, such as yours, will eventually release the floodgates of information from the more constrained organisations that I work with.
Best regards
Roger
...
Maybe review the attached.That has been done. And many issues have been pointed out. Recently an issue with the conservation of energy slide was asked very nicely to Shawyer in an e-mail exchange with rfmwguy, and Shawyer ignored the question entirely. (It was just a few pages back if you missed it)
As I just pointed out and then Rodal provided a link to where Mike McCulloch pointed out the same last year, the arrows on the Conservation of momentum slide indicate Shawyer's confusion with the direction of forces. Cullen's equations if applied blindly and the side walls are ignored result in a force (applied to the cavity walls) in the direction of the "thrust" arrow on that slide. Because from the definition of force, acceleration of an object is in the same direction as the force, the acceleration arrow should also be to the left.
Rather than reposting things that provide no new information, could you address any of the self-contradictions with this theory? Failing that, (since I can think of no way to resolve these contradictions other than simply saying Shawyer is wrong) you could just focus on experiment results and let other people consider theories that at least have a slim chance of explaining any anomalous forces instead of insisting people accept a theory that is equivalent to 1=0.
...I don't see a lone wolf ignoring the comments and input of others.
The miniVNA PRO is on sale for $490. Strange that normally the tiny is a little more expensive, but the PRO has more features, such as bluetooth, battery operation, more dynamic range, 1Hz vs 10Hz, 0dBm vs -6dBm. I guess you are paying for the miniaturization? http://www.hamradio.com/detail.cfm?pid=H0-012128
...I don't see a lone wolf ignoring the comments and input of others.OK, it would help if the "Physicists, Mathematicians and Engineers on both sides of the Atlantic" he refers to would speak in public and write in support of Shawyer's theory, to address several issues. They were absent to defend Shawyer's theory when the New Scientist article was published.
At the moment we would appreciate an answer to the following question: when Shawyer refers to Kinetic Energy to address conservation of energy: how does he measure the velocity to use in his Kinetic Energy expression ? (the kinetic energy changes drastically with frame of reference), and how does he reconcile this frame of reference choice with Special Relativity?
For rockets using propellant exhaust (even relativistic rockets) this issue has been addressed, and there is universal agreement: the effective exhaust velocity of the propellant. The problem for any propellant-less device like the EM Drive is what is the reference velocity?
Has this been addressed?
Thanks
...
The accelerative CofE issue will be soon subjected to experimental data via continual acceleration on rotary test tables as Roger did back in 2006. That data will reveal if the gained angular kinetic energy properly relates to consumed energy - losses or not.
Both QV and MiHsC suggest there are outside energy sources involved to maintain accelerative CofE. Roger says CofE is maintained but not as we perceive and there are no outside energy sources involved nor needed. We should have some prelim data by end 3rd qtr.
Will be exciting to see how this unfolds. Popcorn anyone?
The EmDrive works as claimed.
...
Work backward from that to find what you seek.
snip...
I too started with the mini/tiny VNA but soon the data from the Rf amps forward and reflected real time outputs and the ability to get my Rf gen to do freq sweeps turned it into a backup tool.
Hi Guys,
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 excitation 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.
Paul March, do you have the ability to tune your excitation freq as against thrust generated in real time? If not might be worth a thought as to how to do this to both tune freq for max thrust as well as to map the thrust versus freq bandwidth as against rtn loss versus freq bandwidth. I'm sure there is gold to mine in that data.
Hi Phil
From your NSF posting, I understand that you and another builder have measured thrust bandwidth. The reason why the thrust bandwidth is smaller than the measured cavity bandwidth is because the measured cavity Q is loaded by the Q of the input circuit. In an ideal match, the loaded Q is half the unloaded Q of the cavity.
Classic EmDrive theory however predicts that thrust is dependent on the cavity unloaded Q, as well as the power actually input into the cavity, which is dependent on the match.
Looks like you are both on the right track.
Good to hear your health is improving.
Best regards
Roger
I too started with the mini/tiny VNA but soon the data from the Rf amps forward and reflected real time outputs and the ability to get my Rf gen to do freq sweeps turned it into a backup tool.
What equipment are you using now for RF gen? It would be helpful for DIYers to know so they aren't wasting time and money on tools that aren't good enough in the long-run.
Hi Phil, glad you're feeling better. I think we should probably leave the correct theory to a future date. Mr Shawyer helped and inspired many people. White, McCullough and others took a different theory direction, but we're all on the same team...an obscure and very interesting device that has tremendous ramifications if all the pieces of the puzzle align.
I'll leave the theory to the experts. You and I can build and test to whichever design(s) we like...that's part of the enjoyment. WE pick and choose, not a lab supervisor
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...
Hi Phil, glad you're feeling better. I think we should probably leave the correct theory to a future date. Mr Shawyer helped and inspired many people. White, McCullough and others took a different theory direction, but we're all on the same team...an obscure and very interesting device that has tremendous ramifications if all the pieces of the puzzle align.
I'll leave the theory to the experts. You and I can build and test to whichever design(s) we like...that's part of the enjoyment. WE pick and choose, not a lab supervisor
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...
A quick estimate says the width of the notch 3 dB up from the max. deflection is maybe 100 MHz. I don't know how that would be used to estimate the Q. I think a stronger case for estimating the Q can be made for the absolute maximum deflection of the trace. Any setup will show a narrow 3dB notch but only the best network analyzer will show how deep the notch is. The notch may also be wider with a better instrument. There are many different things that can influence the S11 trace: quality of connectors, cable, and instrument used are some. If the cable is jiggled does the shape of the trace change? Are all the connectors and cable first quality cables and have the connectors all been tightened to the correct torque? The quality of the instrument doing the measurement is unknown if calibration tests are not done. Among the prized possessions of the RF engineers I know are a set of calibration connectors. They include a dead short, an open connector, and terminations of different impedances. Using these calibration connectors the measurements from a NIST certified instrument can be compared to a low cost instrument and corrections made. It's also a good idea to test a filter that has performance plots from the manufacturer on the instrument you are using and see how that measurement compares to what the manufacturer supplied.The 3dB up points from -43dB are probably about a MHz or less wide. The 3dB down points from insertion are wider. Everything was variable as the top and bottom plates were not even soldered, so I didn't get too excited. Just wanted to see generally where peak was.
The 3dB bandwidths have been argued a lot. My test report tried to resolve this by characterizing the shape factor of return loss by creating a ratio of insertion 3dB to peak 3dB bandwidths. This forces a measurement of both bandwidths to avoid confusion. I think Yang measured off peak, EW measured off insertion.
The total span of this image was 2.4 to 2.5 GHz I believe. Insertion return loss should improve once its all soldered. I am using an 8 inch piece of silver plated coax with an SMA from the BeO mounted monopole to the VNA.
Yes, you're correct, a calibrated connector set, cal kits and cables are worth their weight in gold. Especially when working up to and beyond 18 GHz. If my observation tests looks good, I can run down to my old company and have an NIST calibrated sweep done for accuracy. For me, it all hinges on if I can scale the observe effect up giving much more attention to the cavity. If it does, I'll do more. If not, I will retire from building emdrives but will continue to follow developments.
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...
A quick estimate says the width of the notch 3 dB up from the max. deflection is maybe 100 MHz. I don't know how that would be used to estimate the Q. I think a stronger case for estimating the Q can be made for the absolute maximum deflection of the trace. Any setup will show a narrow 3dB notch but only the best network analyzer will show how deep the notch is. The notch may also be wider with a better instrument. There are many different things that can influence the S11 trace: quality of connectors, cable, and instrument used are some. If the cable is jiggled does the shape of the trace change? Are all the connectors and cable first quality cables and have the connectors all been tightened to the correct torque? The quality of the instrument doing the measurement is unknown if calibration tests are not done. Among the prized possessions of the RF engineers I know are a set of calibration connectors. They include a dead short, an open connector, and terminations of different impedances. Using these calibration connectors the measurements from a NIST certified instrument can be compared to a low cost instrument and corrections made. It's also a good idea to test a filter that has performance plots from the manufacturer on the instrument you are using and see how that measurement compares to what the manufacturer supplied.The 3dB up points from -43dB are probably about a MHz or less wide. The 3dB down points from insertion are wider. Everything was variable as the top and bottom plates were not even soldered, so I didn't get too excited. Just wanted to see generally where peak was.
The 3dB bandwidths have been argued a lot. My test report tried to resolve this by characterizing the shape factor of return loss by creating a ratio of insertion 3dB to peak 3dB bandwidths. This forces a measurement of both bandwidths to avoid confusion. I think Yang measured off peak, EW measured off insertion.
The total span of this image was 2.4 to 2.5 GHz I believe. Insertion return loss should improve once its all soldered. I am using an 8 inch piece of silver plated coax with an SMA from the BeO mounted monopole to the VNA.
Yes, you're correct, a calibrated connector set, cal kits and cables are worth their weight in gold. Especially when working up to and beyond 18 GHz. If my observation tests looks good, I can run down to my old company and have an NIST calibrated sweep done for accuracy. For me, it all hinges on if I can scale the observe effect up giving much more attention to the cavity. If it does, I'll do more. If not, I will retire from building emdrives but will continue to follow developments.
Roger has shared with us how SPR measure frustum loaded Q and from that how to calculated unloaded Q as used in his thrust equation.
I do agree with Zen-In that your and mine low cost VNA only do an approximate job and the result from a high price VNA will probably be very different.
However what I have found from my single freq excitation work is it is good enough to get an approximate result, which is good enough to strongly suggest your maggie should trigger bursts of resonance inside the frustum bandwidth and that your polish and general construction accuracy should result is some nicely measurable thrust.
As you now have solid side walls, do a gravity stack, which is as far as I got and using your VNA, try applying some significant weight on different parts of the outer end plate edge to see if this shifts peak rtn loss resonance or changes rtn loss depth. With my 0.5mm thick side walls and 1mm thick end plates, I did see changes, which to me suggests I was altering the parallelism of the end plates by very slightly compressing the side walls at various points as Dr. Rodal suggest can be done with such thin side walls.
You are getting to the fun time as you have a new and very shiny toy to play with and gather good data from. Enjoy. I'm jealous as I can't yet play again with my shiny toy. Well not so shiny at the moment.
...It is not possible to do this modeling without reference to the EmDrive theory developed by Roger and SPR over the years.
The miniVNA PRO is on sale for $490. Strange that normally the tiny is a little more expensive, but the PRO has more features, such as bluetooth, battery operation, more dynamic range, 1Hz vs 10Hz, 0dBm vs -6dBm. I guess you are paying for the miniaturization?
Suggest Dave delete the one where he recommended I purchase it since it was one sale.