Author Topic: EM Drive Developments - related to space flight applications - Thread 8  (Read 1841622 times)

Offline X_RaY

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The 3 boxes are sized such that the diagonal lines are ~ equal length. This illustrates how the dispersion is different for wavelengths along the z axis versus those perpendicular to it.
To me, this looks very similar to the relation of phase velocity versus group velocity, whats changing due to the changing diameter along the central axis of symmetry. ???


It seems you try to describe something like

Q=(2/SkinDepth)(∫Electromagnetic Energy Density dV/ ∫ Electromagnetic Energy Density dA)

while from your viewpoint "Q" stands for "∫Q per λ/2", right?

http://forum.nasaspaceflight.com/index.php?topic=39214.msg1474347#msg1474347
Point 4)
« Last Edit: 11/24/2016 08:02 pm by X_RaY »

Offline mwvp

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Perhaps L-3 became aware of the potential fire hazard of igniting a plasma in a high Q cavity with high power microwaves? IIRC, ~100 MW is the max for an outstanding vacuum in accelerator cavities. If the Q is 10K, and you put 10KW in, there's your 100 MW.

This is a problem that has to be overcome regardless no? What solution would you recommend? Argon environment? Seems like we have to work this out if this unit is to, quite literally, fly.

According to: https://en.wikipedia.org/wiki/Dielectric_gas SF6 can get you 3 - 6 times 30kv/cm breakdown for air, and freon up to 17, pressurized.

From another article I read somewhere, microwave fields can be near double DC or lower frequency fields, because charges don't have time to accelerate.

We need to have someone give us the impedance/fields in the frustrum to know where arcing is likely, and the most power that it can be expected to handle.

From articles I glanced at a couple weeks ago after TT spoke as though he was thinking superconducting cavities with Q's > 10^7 could handle a kilowatt input (dissipated), I saw (IIRC) 100 - 500 MW peak power (not dissipated, stored energy) in hard vacuum. Do a web search for "superconducting cavity accelerator "breakdown voltage"".

New technology will apparently need to be developed to handle high field strengths.

I just wanted to point out, that some engineer at L-3 may have had their manager snicker at them when they asked about putting 100KW into a cavity with Q > 1000. I don't know. There are limits.

Offline Star One

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List of unaddressed or missing issues from the recent EW paper via a poster on Reddit.

https://drive.google.com/file/d/0B6juR48k_XoTREUxc1QycWxwZ2M/view

See what you think?
« Last Edit: 11/24/2016 07:59 pm by Star One »

Offline WarpTech

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The 3 boxes are sized such that the diagonal lines are ~ equal length. This illustrates how the dispersion is different for wavelengths along the z axis versus those perpendicular to it.
To me, this looks very similar to the relation of phase velocity versus group velocity, whats changing due to the changing diameter along the central axis of symmetry. ???


It seems you try to describe something like

Q=(2/SkinDepth)(∫Electromagnetic Energy Density dV/ ∫ Electromagnetic Energy Density dA)

while from your viewpoint "Q" stands for "∫Q per field node (π/2)", right?

All I wanted to do was show that the resonant frequency remains constant, despite the fact that there is dispersion happening in each orthogonal component of the wave. Shawyer's model is based on the dispersion along the z-axis, the "guide wavelength" while @Notsosureofit's model is based on dispersion of the frequency as a whole, which it is assumed behaves like the dispersion of the polar wavefront. I would like to reconcile that the two dispersive forces cancel each other out, leaving ONLY dissipation as the primary component of thrust. :)
« Last Edit: 11/24/2016 08:02 pm by WarpTech »

Offline WarpTech

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List of unaddressed or missing issues from the recent EW paper via a poster on Reddit.

https://drive.google.com/file/d/0B6juR48k_XoTREUxc1QycWxwZ2M/view

See what you think?

I think the EW paper is the best piece of research on the EmDrive that we have seen to date. Being overly critical of every paragraph is time consuming and slows down progress. It is what it is. Risk taking and not-knowing are what drives the ball forward. IMO, EW did a great job, better than anyone else has done at trying to resolve potential errors.

Offline Peter Lauwer

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List of unaddressed or missing issues from the recent EW paper via a poster on Reddit.

https://drive.google.com/file/d/0B6juR48k_XoTREUxc1QycWxwZ2M/view

See what you think?

Good points, most of them. Some I also mentioned earlier.
Science is a way of trying not to fool yourself. The first principle is that you must not fool yourself, and you are the easiest person to fool.   — Richard Feynman

Offline X_RaY

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The 3 boxes are sized such that the diagonal lines are ~ equal length. This illustrates how the dispersion is different for wavelengths along the z axis versus those perpendicular to it.
To me, this looks very similar to the relation of phase velocity versus group velocity, whats changing due to the changing diameter along the central axis of symmetry. ???


It seems you try to describe something like

Q=(2/SkinDepth)(∫Electromagnetic Energy Density dV/ ∫ Electromagnetic Energy Density dA)

while from your viewpoint "Q" stands for "∫Q per field node (π/2)", right?

All I wanted to do was show that the resonant frequency remains constant, despite the fact that there is dispersion happening in each orthogonal component of the wave. Shawyer's model is based on the dispersion along the z-axis, the "guide wavelength" while @Notsosureofit's model is based on dispersion of the frequency as a whole, which it is assumed behaves like the dispersion of the polar wavefront. I would like to reconcile that the two dispersive forces cancel each other out, leaving ONLY dissipation as the primary component of thrust. :)
Todd,
due to EM-field energy to net force conversion it's quite logical that there should be a dissipative component exists in this regard. Better an energy transfer to the thrust component. Pure dissipation, because of resistive losses is also present in a cylindrical conductive cavity, whats needed is a gradient as you describe in your equations, therefore I am with you at this point. :)
« Last Edit: 11/24/2016 08:42 pm by X_RaY »

Offline rq3

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TT, re cavity fabrication ..... if memory serves no more than 4/100s margins? yes?   thnx , FL

??? What does this mean? What are 4/100 margins? Margins of what? Have you a reference to previous posts? Perhaps keep in mind you appear to be asking questions on a public forum of a member who has accomplished a lot of arm waving, prematurely released results without permission to do so, and otherwise posted nothing but noise, unless it was ideas he's slowly absorbed from other's input on this very site. "Magic Happens Inside" strongly implies that some folks don't really understand how to impliment the hardware they fantasize, yet would like to appear to be able to do so. Claims of fabrication, with ball point pen sketches on napkins of multi-thousand dollar hardware just smells "odd", in my not so humble opinion.

If, perchance, you are asking about frustum fabrication tolerances, you might want to include the measurement system involved (English, metric, Klingon). In any case, no published results have determined that fabrication tolerances have any effect whatsoever, except as thay may influence cavity Q, which is well established microwave engineering.

As a microwave engineer, please don't get into the "how do I fabricate a cavity to resonate with my crappy source" discussion again. Even the latest NASA paper is past this one. You need to build the highest Q cavity possible, and then tune the driving microwave source to it, with a control loop that optimizes force. I addressed this almost 2 years ago. Since absolutely no one knows whether this effect exists at all, optimizing for reflection coefficient or any other effect other than the desired one (thrust versus input microwave power) is completely pointless. Maximize the effect until it is out of all conceivable noise, and develop the theory once the effect is proven. To date, the effect is polywater. All results are "down in the grass" (the baseline noise you see on a spectrum analyser due to it's own thermal and phase noise signature).

Shawyer is a microwave engineer too and his results are not in the noise nor are they "polywater"

His peer reviewed results that allow independant 3rd parties to replicate his "results"? I'm probably dating myself, but IIRC there were quite a few peer reviewed methods and means of synthesizing polywater, over a span of something like a decade. So in that repect, you're absolutely right. Polywater was "better science" than the Emdrive.

Offline Peter Lauwer

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List of unaddressed or missing issues from the recent EW paper via a poster on Reddit.

https://drive.google.com/file/d/0B6juR48k_XoTREUxc1QycWxwZ2M/view

See what you think?

I think the EW paper is the best piece of research on the EmDrive that we have seen to date. Being overly critical of every paragraph is time consuming and slows down progress. It is what it is. Risk taking and not-knowing are what drives the ball forward. IMO, EW did a great job, better than anyone else has done at trying to resolve potential errors.

It indeed seems to be the best piece of research in this field. But some important information is missing in the recent article. I advice the Eagleworks team to publish a report with more technical details about the instrumentation (e.g. on researchgate or arxiv), so the work will even gain in quality.
That is how science should work: colleagues are allowed to ask details and criticize the work of others. That certainly doesn't slow down progress.

Cheers,
Peter
Science is a way of trying not to fool yourself. The first principle is that you must not fool yourself, and you are the easiest person to fool.   — Richard Feynman

Offline Star One

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List of unaddressed or missing issues from the recent EW paper via a poster on Reddit.

https://drive.google.com/file/d/0B6juR48k_XoTREUxc1QycWxwZ2M/view

See what you think?

Good points, most of them. Some I also mentioned earlier.

I've looked through them and even with my limited technical knowledge in this area they didn't seem a bad list of issues that's why I cross-posted it.
« Last Edit: 11/24/2016 08:59 pm by Star One »

Offline WarpTech

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All I wanted to do was show that the resonant frequency remains constant, despite the fact that there is dispersion happening in each orthogonal component of the wave. Shawyer's model is based on the dispersion along the z-axis, the "guide wavelength" while @Notsosureofit's model is based on dispersion of the frequency as a whole, which it is assumed behaves like the dispersion of the polar wavefront. I would like to reconcile that the two dispersive forces cancel each other out, leaving ONLY dissipation as the primary component of thrust. :)
Todd,
due to EM-field energy to net force it's quite logical that there should be a dissipation component exists in this regard. Better an energy transfer to the thrust component. Pure dissipation, because of resistive losses is also present in a cylindrical conductive cavity, whats needed is a gradient as you describe in your equations, therefore I am with you at this point. :)

Thanks! In this TE013 mode, we can model it as 3 separate oscillators, all with the same resonant frequency. Based on the wavelengths, the big end would have higher inductance (L), higher resistance (R) and lower capacitance (C). The small end would have lower inductance, lower resistance and higher capacitance. The one in the middle, would be well... in the middle of the range for each component value.

If we use the definition of the decay time as tau ~ L/R. If properly designed there will have 3 different values, hence there is a gradient in the decay time as the energy is dissipated. Charging and discharging should generate a thrust due to this gradient.

I'm just not sure how to determine the momentum of the magnetic flux that is escaping through the voltage drop in the metal.

Offline rfmwguy

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List of unaddressed or missing issues from the recent EW paper via a poster on Reddit.

https://drive.google.com/file/d/0B6juR48k_XoTREUxc1QycWxwZ2M/view

See what you think?

Good points, most of them. Some I also mentioned earlier.

I've looked through them and even with my limited technical knowledge in this area they didn't seem a bad list of issues that's why I cross-posted it.
This was written by eric1600 on Reddit and pretty much sums up critiques I've seen there. A counterpoint should probably be considered as this is a well thought out response and is written in the spirit of scientific discussion without invectives and point of authority argumentation.

Offline SeeShells

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List of unaddressed or missing issues from the recent EW paper via a poster on Reddit.

https://drive.google.com/file/d/0B6juR48k_XoTREUxc1QycWxwZ2M/view

See what you think?

Several relevant points were made, but none that couldn't be answered. Either by data that was left out or by a rerun of the test bed.

Personally I've wondered why a TM212 mode was pushed? When clearly the TE012 mode provided a >5 fold indication of thrust when run. I know now the TE012 mode was hard to keep tuned because of close by resonate modes. Although cost wise a frustum of different dimensions that would have a TE012 or 013 that was sufficiently isolated from accompanying close modes is not that costly or challenging engineering wise.

Dr. White IMHO should have followed the data and brought the thrust levels out from the noise. You could have been recording >600uN instead of the lower 128uN.  I might assume that the reason was is that Dr. White was pushing his theory of Virtual Particle generation and that a TM mode used in particle accelerators might be the main reason why. TE modes won't fit his theory or throw a monkey wrench into theory.
No need to comment on this because it's mostly speculation on my part.

Shell
« Last Edit: 11/24/2016 11:36 pm by SeeShells »

Offline M.LeBel

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I have considered the MHD model for many, many years. My conclusion has been that, the temperature at which electron-positron pairs annihilate each other is in excess of 108 Kelvin. If e-p pairs in the frustum had a density ~1x1012 kg/m3, and a life time of ~10-22 s, the frustum would be vaporized from the heat, faster than dropping it onto the surface of the sun.

The paper in JBIS is saying that it would require a mass of e-p pairs in excess of 105 kg. So the heat and the mass would not go undetected, therefore that's not it.

Regarding the paper you attached, I love this paper! However, at the scale of electrons and quarks, they are constantly undergoing exchange scattering with their counterparts in the QV. At this scale it is possible because the E field exceeds the Schwinger limit, but in the frustum the E field is no where near that limit. So the expectation of producing so many pairs is unreasonable, and I offer that it can't be happening if the frustum is not melting instantly upon their creation.

Todd


Todd:

"My conclusion has been that, the temperature at which electron-positron pairs annihilate each other is in excess of 108 Kelvin."

Again you are making the assumption that the e/p pairs are fully fleshed out in our universe, which does require 0.511 MeV per particle and that would indeed melt the frustum if fully developed.  What Dr. White's QV conjecture posits is that these virtual force carriers can be expressed in our reality with a variable effective mass/energy density that goes from just barely here to fully here at the Schwinger limit energy densities.  Of course the only way to prove this QV conjecture is to test a given frustum design over a broad input power range of four orders of magnitude or greater to see if it generates the COMSOL/QV Plasma code's EW copper frustum's TM010 thrust predictions I posted at NSF.com earlier, or not.

Best, Paul M.

I've read this idea a very long time ago, but I thought it was discredited because I never heard of it again.

If that is the case, a much simpler experiment would be to measure the "linearity" of vacuum permittivity and permeability up to fields strengths equivalent to those in the frustum. Because, any such creation of virtual pairs, or voltage tension between two virtual masses, will change the permittivity and permeability of the vacuum in a measurable way.  How non-linear are vacuum filled capacitors as the field strength approaches 10^7 V/m?

See the attached paper by Urban, which derives these values from the polarizable vacuum. We could probably extend this to apply directly to such an experiment.


Todd:

Great idea and thanks much for the pointer to the Urban paper!  I will read and consider how one might do this on the cheap in my home lab once it is built.

Best, Paul M.

A simple calculation for a parallel plate capacitor with a vacuum dielectric turns out that an electric field of 2.5 x 107 V/m, is not difficult to achieve. For instance, a 1 nF capacitor, is only an area of 10 mm2 with a separation of 8.84 x 10-8 m. This E field strength occurs at only 2.21V!!!! Obviously, if there were significant non-linearity in the vacuum permittivity due to e-p pairs at these field strengths, surely they would've been noticed by now in capacitor manufacturing.

In my view, and my opinion is based on P. W. Milonni's "The Quantum Vacuum", the vacuum "IS" an electromagnetic field. Superimposing a stronger EM field on top of the ZPF, is just raising the energy state of the QV by the number of photons in each state.  The field superimposed on the ZPF, and the ZPF are the same thing, except with a much narrower bandwidth and non-random polarization. If the QV had anything to do with this, then IMO the Casimir effect alone would propel it, but it doesn't. We need to superimpose a stronger field, which we can push against, and that field must be asymmetrically annihilated (dissipated) in order to make it move.

Different perspective ...
IMO the vacuum is an explosive process that started with the Big Bang and is still happening right now i.e. we live in an explosive medium. This explosive process is what we call time and it makes everything in various dynamic combinations.  Any object is therefore of the same nature and replaces locally the time process by logical substitution which explosive deficit away from the object is what we call the gravitational field; a field made of a differential in the rate of time.

When an object is given momentum, its field of explosive deficit is distorted and takes the form of a wave, a pilot wave....  So, we have an object inside an explosive medium of the same nature and whose presence/existence results in a logical substitution of the medium time process a.k.a. gravity.

Assuming that B field is the rate of time dynamically changing (increasing or decreasing) and
the E field is a line along which the rate of time is dynamically changing direction (from increasing to decreasing, or vice-versa)...     
 
WHAT strategy must be used in order to modify the existence field of the object in order to give it the pilot wave shape WITHOUT the usual momentum jerk...

Forget about it! Let’s just drop everything into the “invention machine” ...

http://www.popsci.com/scitech/article/2006-04/john-koza-has-built-invention-machine

 ... and wait for it to spit out the perfect drive while at the same time going around all known patents ...  ;)

Offline M.LeBel

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The 3 boxes are sized such that the diagonal lines are ~ equal length. This illustrates how the dispersion is different for wavelengths along the z axis versus those perpendicular to it.

Food for thought Time ... again   :(

I love those sims charts COMSOL etc.  But, noting being perfect....

What would be the perfect sims softwares?  The “perfect” sims softwares would be the ones where on the graph we see a big huge arrow saying “thrust”.  O.K., we are not there yet! But, could we get a wee bit closer to that perfect chart? From complex modes, swirling electric and magnetic fields, and energy density we are supposed to guess which way the whole thing is going?

Would it be possible (remember, I don’t know what I’m talking about really) to go to some higher level computation in order to get closer to this big arrow? For example, Warptech’s theory is about a differential in the rate of power dissipation. Could this rate be computed ... for, say, a known working set of modes and compare it with the non working modes or settings to see if any significant differences are showing up on the graph; a better visual on a notable asymmetry of sort.. some clues!!!

... Just saying...

Offline Bob Woods

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Today is the Thanksgiving holiday in the US. To all who post here our wishes that you are well and happy in your lives, especially as you debate these challenges to conventional physics.

If you think that sorting out EM claims and dismissals is hard painstaking work, rest assured that we here are arguing both politics and physics over the dinner table. No one has been hurt...yet.  ;)
« Last Edit: 11/25/2016 12:45 am by Bob Woods »

Offline MrJarhead

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The 3 boxes are sized such that the diagonal lines are ~ equal length. This illustrates how the dispersion is different for wavelengths along the z axis versus those perpendicular to it.

Todd - Thanks for this visual aid - it goes a long ways to help some of us laymen understand your hypothesis.  My initial observation was, under your theory, could this same effect be created by taking three (or more) independent cylinder cavities, each having a varying radius and depth so they resonate at similar modes, and stacking them onto one another in a taper fashion?  (To clarify, when I say independent, I mean fully enclosed with separate RF sources)

I would think that depending on the skin depth and material of each cavity, it would be possible to thermally integrate them, so that dissipation could be managed/amplified in interesting ways. 

Anyways, just a quick observation and thought experiment that probably betrays my understanding more than anything :o, but IMO, the answer to this could help clarify what configurations your theory would operate in.

Best regards to everyone who contributes to this effort - it is truly amazing to witness no matter the outcome, now back to lurking ;).

Offline TheTraveller

Roger told me his Flight Thruster had a Qu of 60,000, which seems correct from my spreadsheets Qu calculation based on the assumed Flight Thruster interior dimensions, TE013 mode and 3.85GHz resonance.

Then taking the 1996 Cu room temp Rs as 15,000 uOhm @ 3.85GHz and my latest offered 3uOhm at 3.85GHz, the reduction in Rs is 5,000x. Then the expected Qu would be 6x10^4 * 5x10^3 = 3x10^8 and the expected specific force being 326mN/kW * 5,000 = 1,630N/kW or 166kg/kW. As the Flight Thruster weight was 2.6kg and adding in a 2kg Al cold wick into the LN2 reservoir, will need to levitate say 5kg, which should need 166/5 = 33W to feed into the YBCO thruster.

So a 3.85Ghz 100W Rf amp should be way more than enough and at 33W thermal dissipation, the LN2 boiloff rate will be very low.

All of which suggest doing an experiment to levitate a YBCO, LN2 cooled, Flight Thruster like thruster design is doable, assuming can get 3uOhm at 3.85GHz YBCO applied to ALL interior surfaces.

The doorway to a levitator is again open.

YES I will finish the rotary test rig program and release the data as I consider it vital to have data showing Q dropping or not as acceleration occurs and to plot the cavity energy & momentum loss or not against test rig gained angular KE as velocity increases vs power supply energy supply rate change or not.

Phil
« Last Edit: 11/25/2016 06:23 am by TheTraveller »
It Is Time For The EmDrive To Come Out Of The Shadows

Offline TheTraveller

List of unaddressed or missing issues from the recent EW paper via a poster on Reddit.

https://drive.google.com/file/d/0B6juR48k_XoTREUxc1QycWxwZ2M/view

See what you think?

Several relevant points were made, but none that couldn't be answered. Either by data that was left out or by a rerun of the test bed.

Personally I've wondered why a TM212 mode was pushed? When clearly the TE012 mode provided a >5 fold indication of thrust when run. I know now the TE012 mode was hard to keep tuned because of close by resonate modes. Although cost wise a frustum of different dimensions that would have a TE012 or 013 that was sufficiently isolated from accompanying close modes is not that costly or challenging engineering wise.

Dr. White IMHO should have followed the data and brought the thrust levels out from the noise. You could have been recording >600uN instead of the lower 128uN.  I might assume that the reason was is that Dr. White was pushing his theory of Virtual Particle generation and that a TM mode used in particle accelerators might be the main reason why. TE modes won't fit his theory or throw a monkey wrench into theory.

No need to comment on this because it's mostly speculation on my part.

Shell

My thoughts as well.

Paul's advise, some time ago, should be remembered: "Follow the Data, Theory be Damned".

Of course if the theory also defines the way to do the build, then sometime difficult to follow that advise 100% as you then have nothing to build test devices from.
It Is Time For The EmDrive To Come Out Of The Shadows

Offline TheTraveller

All I wanted to do was show that the resonant frequency remains constant, despite the fact that there is dispersion happening in each orthogonal component of the wave. Shawyer's model is based on the dispersion along the z-axis, the "guide wavelength" while @Notsosureofit's model is based on dispersion of the frequency as a whole, which it is assumed behaves like the dispersion of the polar wavefront. I would like to reconcile that the two dispersive forces cancel each other out, leaving ONLY dissipation as the primary component of thrust. :)
Todd,
due to EM-field energy to net force it's quite logical that there should be a dissipation component exists in this regard. Better an energy transfer to the thrust component. Pure dissipation, because of resistive losses is also present in a cylindrical conductive cavity, whats needed is a gradient as you describe in your equations, therefore I am with you at this point. :)

Thanks! In this TE013 mode, we can model it as 3 separate oscillators, all with the same resonant frequency. Based on the wavelengths, the big end would have higher inductance (L), higher resistance (R) and lower capacitance (C). The small end would have lower inductance, lower resistance and higher capacitance. The one in the middle, would be well... in the middle of the range for each component value.

If we use the definition of the decay time as tau ~ L/R. If properly designed there will have 3 different values, hence there is a gradient in the decay time as the energy is dissipated. Charging and discharging should generate a thrust due to this gradient.

I'm just not sure how to determine the momentum of the magnetic flux that is escaping through the voltage drop in the metal.

Using standard microwave engineering equations for guide wavelength vs mode vs freq vs diameter, the increasing guide wavelength can be plotted big to small end. As seen, the plot is not linear and the guide wavelength starts to get really only as the small end approached cutoff.

Then using Cullen's equation for radiation pressure vs guide wavelength, the decreasing radiation pressure can also be plotted and again is is not linear with decreasing diameter not is it linear with increasing guide wavelength.

While sims like COMSOL and FEKO do show the increasing guide wavelength as the diameter decreases, they don't have the ability, as far as I know, to model the drop in the radiation pressure as the guide wavelength increases.
It Is Time For The EmDrive To Come Out Of The Shadows

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