http://www.popularmechanics.com/science/a18801/3d-printed-wonder-ceramics-wont-shatter/
I want a FRUSTUM from this!
Shell
It would certainly be useful if (a much more rigorous) integration of total energy content could be done at each step of the time marching simulation, so as to have a smooth E(t) plot to summarize how fast the electromagnetic energy builds up, and then compare to what would be expected from Q value, assuming a constant rate of effective power P delivery to the cavity :
E(t)=τ2×P×(1-e-t/τ2) with τ2=Q/ω
http://forum.nasaspaceflight.com/index.php?topic=39004.msg1466547#msg1466547
The rate of power delivery to the frustum is not constant. Far from it.
Initially a resonant cavity being filled looks like a short and almost all the power is rejected with Forward power being almost zero and Reflected power being almost all that was generated.
Ok, get that, so instant constant power delivery from t=0 would need (almost) infinite amplitude initially...
But I can't wrap my head around the distinction between "external Q" and "ohmic Q" and the corresponding β ratio, I'll leave that to the experts...QuoteOk some of the discussion is accelerator cavity related but it still works.
I feel if MEEP is to reflect cavity reality, this 5 x TC fill time, due to Reflected power starting out at almost 100% and dropping to almost 0%, needs to be shown to occur.
Well I don't know what TC we are talking about if there is 2 different Qs involved. Seems like the flattish energy buildup in the initial ~100 time slices (in the long run by Aero) could relate to this initial "refractory" period with almost 100% power reflected, then when we'd have an effective constant power delivery against losses (ohmic + reflected) proportional to energy, that'd give the 1st order (1-e-t/τ2) ...
I somehow get that the cavity is driven by a given amplitude, not by a given forward power, but at some point (as shown on your linked plots) P_forward reaches a plateau. Isn't the corresponding τ1 possibly much below the τ2 of the ensuing charge at (almost) constant P against losses proportional to E ? Sorry for the speculations, not my domain really.
You're right, Traveller, buoyancy wouldn't happen that quick. More importantly, it wouldn't decline that quick.
I would expect buoyancy to propagate at just under 340 m/s. What propagation delay would you expect?
If you are talking balloon like buoyancy, I have no idea how fast any air inside the frustum will heat.., other than by contact with the thermal heating of the frustum itself.
As far as the frustum heating and any internal ballooning or external convection, don't you have to account for how long it take the frustum's heat capacity to be filled before it begins to transfer heat?
Unless you expect that microwave heating of the frustum is uniform, not consistent with Shell's unrecorded observations, any heating of the interior surface of the metal frustum will not be transferred out with 100% efficiency until the frustum is uniformly heated to its full heat capacity.
Shell observed that her side walls felt cool while the endplates felt warm.
Until the whole frustum reaches a stable and uniform temperature, you cannot assume heat will be conducted or dissipated, inside or outside the frustum, in an ideal manner. Some of the initial dissipation will be into the metal frustum itself.

You're right, Traveller, buoyancy wouldn't happen that quick. More importantly, it wouldn't decline that quick.
I would expect buoyancy to propagate at just under 340 m/s. What propagation delay would you expect?
Glenn,
You need to understand that when Iulian pointed the small end down, he measured weight increase on his scale, so the downward force that was generated was greater than the upward buoyancy force.
When you say propagate at 340 m/sec, hey man that is a fast energy wave propagation in air from a internally heated frustum from maggie generated Rf. Bit hard to understand the logic behind that statement. Also you need to quality your statement with the amount of the upward Force that would be generated and in what time frame and response time.
Maybe generate a Glenn upward force overlay as against the measured data that can also explain the very rapid drop in upward force being generated when the maggie was switched off?
Maybe I'm missing something here but how can the upward Force that was being thermally generated (as you suggest) drop so rapidly when the maggie was switched off? This is not a small variation in Force generation.
You're right, Traveller, buoyancy wouldn't happen that quick. More importantly, it wouldn't decline that quick.
I would expect buoyancy to propagate at just under 340 m/s. What propagation delay would you expect?
If you are talking balloon like buoyancy, I have no idea how fast any air inside the frustum will heat.., other than by contact with the thermal heating of the frustum itself.
As far as the frustum heating and any internal ballooning or external convection, don't you have to account for how long it take the frustum's heat capacity to be filled before it begins to transfer heat?
Unless you expect that microwave heating of the frustum is uniform, not consistent with Shell's unrecorded observations, any heating of the interior surface of the metal frustum will not be transferred out with 100% efficiency until the frustum is uniformly heated to its full heat capacity.
Shell observed that her side walls felt cool while the endplates felt warm.
Until the whole frustum reaches a stable and uniform temperature, you cannot assume heat will be conducted or dissipated, inside or outside the frustum, in an ideal manner. Some of the initial dissipation will be into the metal frustum itself.
It might be helpful to find a thermal transfer simulator.
We have conduction, convection and radiation, with conduction dominating the others. Air is a pretty good insulator and will heat a few orders of magnitude slower than copper. However, once a given volume of air is at a higher temperature than ambient, your choice of ideal gas laws will equalize the pressure and cause the "lift" effects very very fast, I would expect the pressure differential to reach equilibrium at something slightly less than the speed of sound. I wouldn't expect it to linger around looking for Elvis before reaching equilibrium with it's environment. While the speed of sound is about 340 m/s the rms speed of air molecules is about 500 m/s at 20 C.
Hence, why would there be an expectation that thermal effects wouldn't happen fast? I think we'd see thermal effect changes in milliseconds.

You're right, Traveller, buoyancy wouldn't happen that quick. More importantly, it wouldn't decline that quick.
I would expect buoyancy to propagate at just under 340 m/s. What propagation delay would you expect?
If you are talking balloon like buoyancy, I have no idea how fast any air inside the frustum will heat.., other than by contact with the thermal heating of the frustum itself.
As far as the frustum heating and any internal ballooning or external convection, don't you have to account for how long it take the frustum's heat capacity to be filled before it begins to transfer heat?
Unless you expect that microwave heating of the frustum is uniform, not consistent with Shell's unrecorded observations, any heating of the interior surface of the metal frustum will not be transferred out with 100% efficiency until the frustum is uniformly heated to its full heat capacity.
Shell observed that her side walls felt cool while the endplates felt warm.
Until the whole frustum reaches a stable and uniform temperature, you cannot assume heat will be conducted or dissipated, inside or outside the frustum, in an ideal manner. Some of the initial dissipation will be into the metal frustum itself.
It might be helpful to find a thermal transfer simulator.
We have conduction, convection and radiation, with conduction dominating the others. Air is a pretty good insulator and will heat a few orders of magnitude slower than copper. However, once a given volume of air is at a higher temperature than ambient, your choice of ideal gas laws will equalize the pressure and cause the "lift" effects very very fast, I would expect the pressure differential to reach equilibrium at something slightly less than the speed of sound. I wouldn't expect it to linger around looking for Elvis before reaching equilibrium with it's environment. While the speed of sound is about 340 m/s the rms speed of air molecules is about 500 m/s at 20 C.
Hence, why would there be an expectation that thermal effects wouldn't happen fast? I think we'd see thermal effect changes in milliseconds.
http://www.popularmechanics.com/science/a18801/3d-printed-wonder-ceramics-wont-shatter/
I want a FRUSTUM from this!
Shell
...
A metal surface will not heat up and transfer heat in milliseconds. I can heat cooking oil to a couple hundred degrees C on a stove top burner. Take an empty pan at 24 degrees C, place it over a burner and measure the temperature on the inside surface of the pan... Even using a pan composed of a single layer of stainless steal it takes around 10 seconds to raise the temperature by 20 degrees C... And the temperature of the side wall of the pan, Rises even slower inside or out.
That is why I am saying that thermal effects would be delayed, or more gradual.., even more so on the declining side, since unless you have heated the entire pan or frustum to a uniform temperature, the temperature of the whole will still be trying to equalized.
Ballooning for a frustum depends on either out gassing which results in a lower pressure inside than outside or if sealed that the frustum actually expands enough, to alter its displacement... Either one again would be far slower than thermal conductivity.
External convection very much depends on how fast, in reality heat is transferred through the frustum walls... And as demonstrated by the final conclusions re: The Pioneer Anomaly, exactly how and where heat is dissipated will affect radiating thermal thrust and should affect any convection currents.
The thermal issues are anything but simple or ideal.
It has been argued that the anomalous results found by NASA's Brady et.al for microwave cavities (that supposedly act as a propellant-less thruster) cannot be due to thermal effects because a) the temperature increase would need to amply exceed several degrees C to be explained by thermal effects and b) thermal effects take place too slowly (minutes) and cannot explain the impulsive response of the thrust pendulum exhibiting a rise to full amplitude in half the pendulum's period (rise to full amplitude in little over 2 seconds). These (analytically unsupported) arguments are invalidated here: a thermo-mechanical effect (thermal buckling) is shown that occurs in less than 1 second (for the copper thickness that has been argued as employed for the microwave cavity), with a temperature increase of a degree C or less and that results in forces of the same magnitude (microNewtons) as reportedly measured by NASA.
). A small community of researchers continues to investigate cold fusion, now often preferring the designation low-energy nuclear reactions (LENR)...Since cold fusion articles are rarely published in peer-reviewed mainstream scientific journals, they do not attract the level of scrutiny expected for mainstream scientific publications.
Can we please keep the LENR out of here? We already have enough critics.
LENR is very real as is EmDrive.
2016 is going to be a very interesting year as a lot of folks duck for cover as 2 techs are proven to be very real and game changing.
For EmDrives to make a really serious dent in space, the tech needs a lot of electrical energy. Really more than any existing space power tech can deliver. Do the math. Check it out. When you replace chem propulsive energy with EmDrive kinetic energy from electricity you need a lot electrical power to make it work. EmDrive electrical energy to kinetic energy conversion efficiency is VERY LOW. In the process of generating the kinetic a LOT OF HEAT will be generated.
So no LENR direct electrical energy generation in space and the EmDrive in space may die a slow death as chem energy can do the job at a better efficiency.
And LENR is outside of the scope of this forum.
Do the efficiency maths. Without the high energy density direct LENR to electricity generation efficiency that can deliver, there is little chance of EmDrive delivering space.
Anyway well past my bed time. Night all.
While I know I should just let this die... I have to respond.
While I am open to LENR hopefully delivering on its promise. It isnt neccessary. If EmDrive pans out. We will start powering them with Fuel Cells, and solar since our initial scope will be Earth LEO/GEO, Moon, Mars, Venus. So whatever we can do with just those energy sources will be done. At the same time. Nuclear Fission reactors will finally gain yet another reason to be fast tracked to the front of the deep space energy generation line. Since heat management is bound to be something we will have to deal with anyway. We might as well build a heat rejection system that can handle fission/fusion reactors that generate electricity from thermal conversion.
So no LENR isnt the only way we get the solar system or stars in our galaxy. Even though it would be a pretty sweet solution if it materialized as promised.
Recall fuel cells are energy storage systems (like batteries) not long-term energy production systems (like solar/nuclear systems).
This is a very custom design job. A very rough sketch of my design is attached.
This design needs no circulator and Rf dummy load as the real time Rf environment is monitored at least 100 times a second and will never allow the Rf amp to be over stressed. Rf power is programmed from approx 200mW to 100W with real time Forward and Reflected power feedback. If reflected power exceeds programmed limits, power output levels are dropped back in real time.
https://www.researchgate.net/publication/268804028_NASA%27S_MICROWAVE_PROPELLANT-LESS_THRUSTER_ANOMALOUS_RESULTS_CONSIDERATION_OF_A_THERMO-MECHANICAL_EFFECTQuote from: RodalIt has been argued that the anomalous results found by NASA's Brady et.al for microwave cavities (that supposedly act as a propellant-less thruster) cannot be due to thermal effects because a) the temperature increase would need to amply exceed several degrees C to be explained by thermal effects and b) thermal effects take place too slowly (minutes) and cannot explain the impulsive response of the thrust pendulum exhibiting a rise to full amplitude in half the pendulum's period (rise to full amplitude in little over 2 seconds). These (analytically unsupported) arguments are invalidated here: a thermo-mechanical effect (thermal buckling) is shown that occurs in less than 1 second (for the copper thickness that has been argued as employed for the microwave cavity), with a temperature increase of a degree C or less and that results in forces of the same magnitude (microNewtons) as reportedly measured by NASA....
http://www.popularmechanics.com/science/a18801/3d-printed-wonder-ceramics-wont-shatter/
I want a FRUSTUM from this!
Shell
http://www.popularmechanics.com/science/a18801/3d-printed-wonder-ceramics-wont-shatter/
I want a FRUSTUM from this!
Shell
Yes, let's see if this process can be adapted for YBCO! But for now, I am going to keep my eyes on MgB2. For the time being, it's only my eyes, as I can't get my hands on any until my money arrives...which should be soon!
http://www.popularmechanics.com/science/a18801/3d-printed-wonder-ceramics-wont-shatter/
I want a FRUSTUM from this!
Shell
Yes, let's see if this process can be adapted for YBCO! But for now, I am going to keep my eyes on MgB2. For the time being, it's only my eyes, as I can't get my hands on any until my money arrives...which should be soon!
[/quote。 Cooling MgB2 cavity is very difficult
http://www.popularmechanics.com/science/a18801/3d-printed-wonder-ceramics-wont-shatter/
I want a FRUSTUM from this!
Shell
Yes, let's see if this process can be adapted for YBCO! But for now, I am going to keep my eyes on MgB2. For the time being, it's only my eyes, as I can't get my hands on any until my money arrives...which should be soon!I have a friend who is a high temperature superconducting engineer, has been promoting his design of YBCO thin film resonator