Could you describe your rig when you are running calibration pulses? Does disconnecting all of the batteries on the rig have any effect on the noise profile during calibration?
For your calibration pulses, are you using a permanent magnet on the torsion arm, and an electromagnet nearby? Would it be possible to physically move the electromagnet after the calibration pulse? A moving permanent magnet can induce currents in a nearby electromagnet, so I was wondering if that might be one of the noise sources. Increasing the size of the air gap after the calibration pulse finishes would help test whether the electromagnet was having any effect on the noise.
Does the noise profile look different if the calibration pulse is stronger/weaker?
With everything unplugged and unpowered, I still get the noise. The calibration pulse is simply a small electromagnet outside of the enclosure. Inside the enclosure attached to the pendulum is a small aluminum arm that extends to 4cm away from the calibration coil. Attached to this arm is a small ferromagnetic screw. I use the electromagnet at a known distance and current to exert a force on the screw. Yes, I still get the noise even if the calibration coil is taken away.
I also performed a test increasing the air-gap. See below. The little spike in the middle in me moving the coil. This was one of the better runs.
This is probably the dumbest thing I've ever said but have you tried adding the opposite of the noise signal in a feedback loop to see what happens?
If someone wants to try, here are the excel files. If there is an easy way to do that in excel, please let me know the formula I should use.
IMO, you should present what you have. Compared to what Prof. Tajmar presented last year on the MEGA, you've done a helluva lot more work and have a lot more data than he had to present. I think a lot of people will really appreciate all the work you put into this, and how much difficulty there is in eliminating the noise.
IMO, you should present what you have. Compared to what Prof. Tajmar presented last year on the MEGA, you've done a helluva lot more work and have a lot more data than he had to present. I think a lot of people will really appreciate all the work you put into this, and how much difficulty there is in eliminating the noise.
Thank you, but I have already sent the cancellation notice to Heidi Fearn. She was very gracious in her reply. There was a late addition, so there shouldn't be issues with the schedule. She said I would be invited to present at the next conference in Estes Park 2018 to give me more time with the experiment.
Could you describe your rig when you are running calibration pulses? Does disconnecting all of the batteries on the rig have any effect on the noise profile during calibration?
For your calibration pulses, are you using a permanent magnet on the torsion arm, and an electromagnet nearby? Would it be possible to physically move the electromagnet after the calibration pulse? A moving permanent magnet can induce currents in a nearby electromagnet, so I was wondering if that might be one of the noise sources. Increasing the size of the air gap after the calibration pulse finishes would help test whether the electromagnet was having any effect on the noise.
Does the noise profile look different if the calibration pulse is stronger/weaker?
With everything unplugged and unpowered, I still get the noise. The calibration pulse is simply a small electromagnet outside of the enclosure. Inside the enclosure attached to the pendulum is a small aluminum arm that extends to 4cm away from the calibration coil. Attached to this arm is a small ferromagnetic screw. I use the electromagnet at a known distance and current to exert a force on the screw. Yes, I still get the noise even if the calibration coil is taken away.
I also performed a test increasing the air-gap. See below. The little spike in the middle in me moving the coil. This was one of the better runs.
Basic principles
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More advanced, so called two-phase lock-in-amplifiers have a second detector, doing the same calculation as before, but with an additional 90° phase shift. Thus one has two outputs: {\displaystyle X=V_{\text{sig}}\cos \theta } {\displaystyle X=V_{\text{sig}}\cos \theta } is called the "in-phase" component, and {\displaystyle Y=V_{\text{sig}}\sin \theta } {\displaystyle Y=V_{\text{sig}}\sin \theta } the "quadrature" component. These two quantities represent the signal as a vector relative to the lock-in reference oscillator. By computing the magnitude (R) of the signal vector, the phase dependency is removed:
The phase can be calculated from
Is 3 uN really a "significant" noise source.
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The first I will suggest is a low frequency filter. Basically a capacitor and inductor/resistor circuit set up so that current flowing in the circuit filters different frequencies.
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Another option using a frequency might be a lock in amplifier.
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I'm thinking that I will back out of the advanced propulsion workshop in November. I've been working non-stop for a week now trying to collect good data and I can't seem to nail down the noise problem
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I'm thinking that I will back out of the advanced propulsion workshop in November. I've been working non-stop for a week now trying to collect good data and I can't seem to nail down the noise problem (see image below). I can easily detect forces below 3uN if the pendulum is completely still, but that is seldom the case - which is very frustrating. Just when I think I have solved the problem and get a clean run, the noise returns the next day with the same vigor. There has to be something fundamentally wrong that i'm missing, or this is the reason these experiments are performed in a vacuum! In order to minimize the noise further I would need to increase the torsional spring constant and get a laser displacement sensor with higher resolution - which requires an ADC with higher resolution. In other words, another major retooling and expense.
There were emails this weekend about how they may have too many presentations on the emdrive this year. Without good clear data, I wouldn't have much to add. It's also just a hobby for me and the idea of presenting this material in front of a bunch of professional scientists is very intimidating. I know a cancellation means I probably won't be invited back, but I can't present this kind of data and expect it to be taken seriously. There is also a deadline for a final paper that I just can't commit to. I should have never accepted the offer to present to begin with. I am deeply sorry to those who recommended me and everyone counting on me.
I will continue working, as it brings me joy and satisfaction, just at a slower pace.
My Best,
Jamie
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Abstract
A gedankenexperiment was considered to compare a hypothetical thruster that used no reaction mass to propulsion methods currently in use. A brief discussion of previous research work done on closed resonant cavity thrust devices was conducted. Using the previous work as a template, a simulation plan was devised. Computational models of resonant microwave cavities were constructed and investigated using COMSOL software. These COMSOL simulations were verified against known analytical solutions using Matlab software as a computational tool. Multiphysics simulations were created to study the microwave heating environment of the resonant cavities. From the COMSOL study outputs, the electromagnetic field magnitude, temperature, surface resistive losses, volume resistive losses, quality factor, and energy contained in the electric field were presented and discussed. The disagreements between the computational model and real-world resonant cavities were also presented and discussed.
It is not expected that the failure to accurately compare COMSOL’s spherical resonant cavity model to that represented by the analytical solution will affect the cavities that are the focus of this thesis.
There is either a significant noise source, or a small noise source exciting a very poorly damped (and complex) mode of oscillation. Try a second damper to eliminate oscillations on axes through the damper, or failing that make the damper paddle much longer with the same total damping. Sorry to be broken record, but if you are desperate you might as well try it. No garauntee it will work.
Jamie, just shooting in the dark, but did you consider that the noise you're observing may be somewhat picked up by the cabling ? Also, if I'm not wrong, the computer and the analyzer are sitting on the arm, I suppose either or both have an internal oscillator used for the clock, and that may generate some noise, same goes for USB signals.
Not willing to teach you how to run your business, just throwing some ideas on the table in an attempt to help
Jamie, just shooting in the dark, but did you consider that the noise you're observing may be somewhat picked up by the cabling ? Also, if I'm not wrong, the computer and the analyzer are sitting on the arm, I suppose either or both have an internal oscillator used for the clock, and that may generate some noise, same goes for USB signals.
Not willing to teach you how to run your business, just throwing some ideas on the table in an attempt to help
Agree. Though using an on-board computer can make it easier to automate the experiment, it also potentially introduces noise. When I did my experiment, I designed an optically activated solid stat switch that does not have internal oscillator. Everything is static. Maybe it is worth to move the computer to the framework, from where it uses laser or flashlight to control the experiment equipped with optically activated (or RF controlled) solid stat switches.
Something is causing the pendulum to move in unexpected ways. It has too many degrees of freedom in my opinion and needs to be constrained to the one we are measuring.
The plan is to remove the piano wire and replace it with flexure bearings. I have to be careful that I use flexure bearings that do not exceed by much the current 0.00326 lb-in per degree torsion spring constant but can still support ~25lbs. That means I can use either one E-10 c-flex bearing (0.0036 lb-in per degree, 36.5lbs axial load capacity) or two D-10 bearings (0.0018 lb-in per degree, 22.7 lbs axial load capacity). I will also be replacing the rectangular damping fluid reservoir with something circular.
I ordered the three flexure bearings today, as they are not very expensive, but installing them is going to require a couple of weeks.
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Rodal then disproved TT (who was reporting Shawyer's email message about the problem of COMSOL when applied to the EmDrive, especially the controversial "cut-off rule" of a cylindrical waveguide applied to a closed cavity as a key for thrust generation) with a peer-reviewed paper validating the precision and power of COMSOL, but this paper treated precisely of rectangular cavities, which COMSOL does not have any problem with according to Pennington.
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Rodal then disproved TT (who was reporting Shawyer's email message about the problem of COMSOL when applied to the EmDrive, especially the controversial "cut-off rule" of a cylindrical waveguide applied to a closed cavity as a key for thrust generation) with a peer-reviewed paper validating the precision and power of COMSOL, but this paper treated precisely of rectangular cavities, which COMSOL does not have any problem with according to Pennington.
...1) My paper on cut-off solutions (attached below) had a comparison with an exact solution for a truncated conical cavity, and not for a rectangular cavity. Actually, I did not perform any comparisons for rectangular cavities.
The message you are quoting is one of many I wrote addressing this issue, there are stronger reasons to challenge TT's statements about the appropriateness of numerical solutions than the message quoted.
2) Finite Element Methods should not be discussed as "black boxes", preferably in academic graduate research one should write the numerical routines which presumes having access to change the code.
3) COMSOL uses the Galerkin solution method, which is one the weakest methods of numerical solution. Particularly if one suspects a numerical code, one should use more than one code for comparison, particularly in academic research. For example, one should use excellent codes like ABAQUS, and ADINA that have a strong theoretical basis. Most importantly academic research should address address convergence of the numerical scheme.
4) In this case (the EM Drive) the pertinent comparison between exact solutions and numerical methods should be for a truncated conical cavity (and not for spherical or rectangular cavities). A comparison with a cylindrical cavity is also pertinent, as most EM Drive designs have been close to cylindrical. A comparison with a spherical geometry is the least pertinent (as readily apparent from an understanding of the resonant modes in a perfectly symmetric spherical cavity as compared to an asymmetric resonant cavity like the EM Drive).