QuoteI thought Shell only had one side connected, and the other one floating... Has she chosen the right side?
First off good luck. To address your question both of my endplates are electrically connected. The large bottom plate is soldered and then a bead of silver epoxy to seal it airtight.
The small top endplate floats is right but it floats on a Beryllium flexible gasket.
Here are a few on ebay.
http://www.ebay.com/sch/i.html?_odkw=Beryllium+Copper+EMI+Gasket+Strip&_osacat=0&_from=R40&_trksid=m570.l1313&_nkw=Beryllium+Copper+EMI+Gasket+Strip&_sacat=0
(mod corrected url)
This does several things. Allows me to keep the small endplate conductive to the frustum walls while sliding up and down inside of the tune chamber and also allows heated air out of the cavity through the gaps. The very top of the tune cavity is sealed off and I have a small airline connected to it running back down the beam to vent heated air.
I really want to be able to tune the chamber through the resonance points plotting any thrusts I get and put this cutoff or no cutoff issue to bed. This means an extended full power run. Currently I've been working on a little DC variable speed motor on the end of the micrometer at the large end to slowly slide the small plate up and down.
Good luck on your run and your data. Very nice work.
Shell
....
If anyone knows why this frustum should not be producing thrust then speak now or forever hold your peace.
Ladies and Gentleman, you can now make your bets. (I have already simulated mode frequency shifts for difference thicknesses of HDPE disks at the small end, so this gives a good hint as to what my own prediction for this upcoming test is…)
Here is my bet: No thrust. Why? Because I believe EmDrive effect does not exist.
And my bet, while the same, is slightly more optimistic: it seems that the only existing report to date of somebody being able to observe thrust from an RF cavity without dielectric and without using 700W ofheatDC powerRF magnetron energy is Cannae Superconducting. They have (presumably) got like 10 mN from 10W at 10M Q. Well, if the effect does exist and it scales linearly with Q then the most optimistic estimate for one operating with 30W and 10K unloaded Q is ... ~30 uNThis is most likely below the resolution of my setup.
However, I am now pretty convinced (ok, not yet but I most likely will be after the next test) that any effects on the order of ~400 mN / KW cannot be replicated under pure single freq RF power using solely information available in the public domain. Note I am not saying they don't existI am saying there is no compelling reason to believe that they exist as of today...
QuoteI thought Shell only had one side connected, and the other one floating... Has she chosen the right side?
First off good luck. To address your question both of my endplates are electrically connected. The large bottom plate is soldered and then a bead of silver epoxy to seal it airtight.
The small top endplate floats is right but it floats on a Beryllium flexible gasket.
Here are a few on ebay.
http://www.ebay.com/sch/i.html?_odkw=Beryllium+Copper+EMI+Gasket+Strip&_osacat=0&_from=R40&_trksid=m570.l1313&_nkw=Beryllium+Copper+EMI+Gasket+Strip&_sacat=0
(mod corrected url)
This does several things. Allows me to keep the small endplate conductive to the frustum walls while sliding up and down inside of the tune chamber and also allows heated air out of the cavity through the gaps. The very top of the tune cavity is sealed off and I have a small airline connected to it running back down the beam to vent heated air.
I really want to be able to tune the chamber through the resonance points plotting any thrusts I get and put this cutoff or no cutoff issue to bed. This means an extended full power run. Currently I've been working on a little DC variable speed motor on the end of the micrometer at the large end to slowly slide the small plate up and down.
Good luck on your run and your data. Very nice work.
Shell
Shell,
Any chance you have a drawing of your setup? I am trying to keep a mental compilation of all the details for it based on your posts and pictures, but it would be so much easier if there were a drawing...
Thanks!
As Thane Heins' patent agent and someone with a loose MIT connection to Markus Zahn, I was of course very gratified to see "Rodal" post a citation to the newly-issued US#9,230,730.
It took me some time to see how Mr. Heins' claims, though seemingly fanciful, were grounded in genuine innovation. The fact that I knew him in high school helped me to suspend disbelief.
I encourage everyone to also inspect the as-yet-unexamined patent application for the "Perepiteia" itself:
www.google.com/patents/US20140111054
Both above patent documents include competent explanations of what might be termed "the Heins effect." The complete explanation took a great deal of time and work and is an ongoing project.
Yes Virginia, there are undiscovered inventions waiting to be found by the unlikeliest of people, in the unlikeliest of places.
Les Virany BSEE MIT, Registered Patent Agent
Licensed to teach physics in the state of MA.
fantastic to see you here!
Ladies and Gentleman, you can now make your bets. (I have already simulated mode frequency shifts for difference thicknesses of HDPE disks at the small end, so this gives a good hint as to what my own prediction for this upcoming test is…)
Cannae.com FYI only - A tangential type of EMDrive using non-frustum type cavity.
Their website has been down for a few weeks. Status of their website: http://www.icann.org/epp#clientRenewProhibitedAre they still in business ?
This is not the first time that we have posts about their website being down. Website being down like this does not look good...
As Thane Heins' patent agent and someone with a loose MIT connection to Markus Zahn, I was of course very gratified to see "Rodal" post a citation to the newly-issued US#9,230,730.
It took me some time to see how Mr. Heins' claims, though seemingly fanciful, were grounded in genuine innovation. The fact that I knew him in high school helped me to suspend disbelief.
I encourage everyone to also inspect the as-yet-unexamined patent application for the "Perepiteia" itself:
www.google.com/patents/US20140111054
Both above patent documents include competent explanations of what might be termed "the Heins effect." The complete explanation took a great deal of time and work and is an ongoing project.
Yes Virginia, there are undiscovered inventions waiting to be found by the unlikeliest of people, in the unlikeliest of places.
Les Virany BSEE MIT, Registered Patent Agent
Licensed to teach physics in the state of MA.
I'll post you something but I've got company banging at the door. Give me a couple hours....
Standard WR340 Waveguides Coax>Waveguide 1/4 Wl antenna @2.47GHz
http://imgur.com/gzwV3yu
http://imgur.com/Kgkddmn
LENGTH-x = 0.1761 m, BIG DIA.-y,z = 0.3077 m, Small dia. = 0.1727 m
I'll dig out the drawings later....
Dr. Rodal: thanks very much for correcting my misunderstanding re: frustrum wall currents, I appreciate the time you took to do so.
Would Ohmic heating still need to reconcile with the (induced) wall currents? More directly, can you give us all the scale of the expected wall currents in a 100W RF frustrum? I'm reluctant to re-visit the back of my envelope for a while, as you might imagine. I followed the link to the post you gave, but didn't spot anything which looked like it would answer the question directly.
R.
is:arbitrarily large steady electric currents
since the large electric currents that can be achieved with current superconducting cables, roughly of order 10^4 A, will generate extremely weak space-time curvature, it will be necessary to amplify the signal by forcing light to perform numerous round trips in the artifi cially generated gravitational fi eld.
Dr. Rodal: thanks very much for correcting my misunderstanding re: frustrum wall currents, I appreciate the time you took to do so.
Would Ohmic heating still need to reconcile with the (induced) wall currents? More directly, can you give us all the scale of the expected wall currents in a 100W RF frustrum? I'm reluctant to re-visit the back of my envelope for a while, as you might imagine. I followed the link to the post you gave, but didn't spot anything which looked like it would answer the question directly.
R.I could write some Wolfram Mathematica code to calculate the eddy currents in the EM Drive, but I would need to have some motivation to do it. Motivation not to spend the time to do itis:
...
<some very good arguments here>
...
If you have some counterarguments, to motivate one to calculate the eddy currents, please let me know
Dr. Rodal: thanks very much for correcting my misunderstanding re: frustrum wall currents, I appreciate the time you took to do so.
Would Ohmic heating still need to reconcile with the (induced) wall currents? More directly, can you give us all the scale of the expected wall currents in a 100W RF frustrum? I'm reluctant to re-visit the back of my envelope for a while, as you might imagine. I followed the link to the post you gave, but didn't spot anything which looked like it would answer the question directly.
R.I could write some Wolfram Mathematica code to calculate the eddy currents in the EM Drive, but I would need to have some motivation to do it. Motivation not to spend the time to do itis:
...
<some very good arguments here>
...
If you have some counterarguments, to motivate one to calculate the eddy currents, please let me know
Or I can post a COMSOL plot of surface current density at 100W input if it helps... That recent colorful plot of surface _power_ density was for either 1W or 10W of input power (I just don't remember the settings as it was simulated a while ago)...
Dr. Rodal and others -
Attached find my attempt, with SeeShell's guidance, to model the geometry of Tajmar's frustum. I have labelled the sections so that we can identify them for discussion.
I have made several guess: Like "What is the height of the feed and coupler sections?" I'm assuming that the width is 1/2 the height as is common for waveguides, and Shell extracted the section lengths from the image. I am still in doubt about the length of the WR 340 but Shell assures me that it is a commercial part and I'm using those dimensions. But the antenna doesn't seem to me to be the right distance from the end of the WR 340 being 0.021336 meters instead of 1/4 wavelength which is about 0.03 meters.
One other item in question is regarding a rectangular z-choke. Did Tajmar use one as Yang did, and if he did, where was it located?
In any event the fields are not forming quickly, if they ever will. The attached two gif's are 10 frames from one cycle at the end of a 64 cycle run. I haven't tried to make a resonance run because I think there is still some tweaks needed to the model.
We iterated our design several times by consulting with R. Shawyer to be as representative as possible. Our final tapered cavity design had an
internal top radius of 38.5 mm, a
bottom radius of 54.1 mm and a
height of 68.6 mm
as well as a side entrance for the microwaves as shown in Fig. 2. The cavity was made out of three copper pieces with a wall thickness of 3 mm where the lower and middle part as well as the side flange were hard soldered using silver and the top part was able to adapt its position in order to optimize for a high Q factor. A standard WR340 waveguide was then used to connect the magnetron to the EMDrive
Dr. Rodal and others -
Attached find my attempt, with SeeShell's guidance, to model the geometry of Tajmar's frustum. I have labelled the sections so that we can identify them for discussion.
I have made several guess: Like "What is the height of the feed and coupler sections?" I'm assuming that the width is 1/2 the height as is common for waveguides, and Shell extracted the section lengths from the image. I am still in doubt about the length of the WR 340 but Shell assures me that it is a commercial part and I'm using those dimensions. But the antenna doesn't seem to me to be the right distance from the end of the WR 340 being 0.021336 meters instead of 1/4 wavelength which is about 0.03 meters.
One other item in question is regarding a rectangular z-choke. Did Tajmar use one as Yang did, and if he did, where was it located?
In any event the fields are not forming quickly, if they ever will. The attached two gif's are 10 frames from one cycle at the end of a 64 cycle run. I haven't tried to make a resonance run because I think there is still some tweaks needed to the model.This is the information I'm aware of:
* Between the Cavity and the waveguide Tajmar used an adapter.
Following are the dimensions in the latest corrected version of Tajmar's EM Drive paper:
http://bit.ly/1h4E0RzQuoteWe iterated our design several times by consulting with R. Shawyer to be as representative as possible. Our final tapered cavity design had an
internal top radius of 38.5 mm, a
bottom radius of 54.1 mm and a
height of 68.6 mm
as well as a side entrance for the microwaves as shown in Fig. 2. The cavity was made out of three copper pieces with a wall thickness of 3 mm where the lower and middle part as well as the side flange were hard soldered using silver and the top part was able to adapt its position in order to optimize for a high Q factor. A standard WR340 waveguide was then used to connect the magnetron to the EMDrive
...The dimensions I am using, from FluxCapacitor's post give the same diameters but a greater height of 72.8 mm. Which set of dimensions do you suppose is correct?
Looking at the images in the paper from Tajmar, it looks like the cavity tested was not the same as the prototype cavity commonly illustrated and which I based the model geometry on. Assuming that the cavity imaged inside of the vacuum chamber was the one tested. .....
aero
Dr. Rodal: thanks very much for correcting my misunderstanding re: frustrum wall currents, I appreciate the time you took to do so.
Would Ohmic heating still need to reconcile with the (induced) wall currents? More directly, can you give us all the scale of the expected wall currents in a 100W RF frustrum? I'm reluctant to re-visit the back of my envelope for a while, as you might imagine. I followed the link to the post you gave, but didn't spot anything which looked like it would answer the question directly.
R.I could write some Wolfram Mathematica code to calculate the eddy currents in the EM Drive, but I would need to have some motivation to do it. Motivation not to spend the time to do itis:
...
<some very good arguments here>
...
If you have some counterarguments, to motivate one to calculate the eddy currents, please let me know
Or I can post a COMSOL plot of surface current density at 100W input if it helps... That recent colorful plot of surface _power_ density was for either 1W or 10W of input power (I just don't remember the settings as it was simulated a while ago)...
Yes, it would be great if you could show the COMSOL plot of surface current density at 100W input
Dr. Rodal: thanks very much for correcting my misunderstanding re: frustrum wall currents, I appreciate the time you took to do so.
Would Ohmic heating still need to reconcile with the (induced) wall currents? More directly, can you give us all the scale of the expected wall currents in a 100W RF frustrum? I'm reluctant to re-visit the back of my envelope for a while, as you might imagine. I followed the link to the post you gave, but didn't spot anything which looked like it would answer the question directly.
R.I could write some Wolfram Mathematica code to calculate the eddy currents in the EM Drive, but I would need to have some motivation to do it. Motivation not to spend the time to do itis:
...
<some very good arguments here>
...
If you have some counterarguments, to motivate one to calculate the eddy currents, please let me know
Or I can post a COMSOL plot of surface current density at 100W input if it helps... That recent colorful plot of surface _power_ density was for either 1W or 10W of input power (I just don't remember the settings as it was simulated a while ago)...
Yes, it would be great if you could show the COMSOL plot of surface current density at 100W input
Ok, I created a folder where all relevant outputs (electrical and magnetic fields, surface current density and surface power losses) for one particular frustum at one specific mode (TE012) at 100W input are saved. This can likely serve as a reference for anyone wondering about "what order of magnitude <something> is inside the EmDrive cavity"? There is also a ReadMe.txt in the same folder with description.
Here's the link: https://drive.google.com/open?id=0B3jbXEyEMvU8ZEFJV0pwNUdyaEU
ReadMe.txt:
D small: 158 mm
D big: 264 mm
L_center: 204 mm
Freq: 2323.062 [MHz]
S11 (dB): -31.59
Q factror (unloaded): 75152
Dissipated Power (W): 99.27
Lumped port impedance: 52.39-0.97i
Surface current density jfyi: https://drive.google.com/file/d/0B3jbXEyEMvU8dnpWUDBGYWpESlk/view?pref=2&pli=1
(Sorry, image does not show with "Img" tag. File / resolution may be too big?)
Dr. Rodal and others -
Attached find my attempt, with SeeShell's guidance, to model the geometry of Tajmar's frustum. I have labelled the sections so that we can identify them for discussion.
...