The confusing thing is that, however EW reported zero thrust without dielectric
Nice video of the Flight Thruster which shows the "Tuning Port":
https://www.youtube.com/watch?v=KUX8EWxmS3k&feature=youtu.be&t=553
Seems to be very light, so it is probably Aluminum based.
The confusing thing is that, however EW reported zero thrust without dielectric
That is not correct.
and measured no significant net thrust.
my recollection is that later discussion by Star-Drive at NSF was to the effect that later measurements in another measuring device, in another mode shape (not the TE012 mode shape discussed in that paragraph in the Brady report), under ambient pressure, may have resulted in a force measurement without a dielectric, but that the measurements with a dielectric still gave greater force/inputPower measurements than without the dielectric, at NASA.
my recollection is that later discussion by Star-Drive at NSF was to the effect that later measurements in another measuring device, in another mode shape (not the TE012 mode shape discussed in that paragraph in the Brady report), under ambient pressure, may have resulted in a force measurement without a dielectric, but that the measurements with a dielectric still gave greater force/inputPower measurements than without the dielectric, at NASA.
Excited mode is not relevant. EW has observed force generation without a dielectric.
my recollection is that later discussion by Star-Drive at NSF was to the effect that later measurements in another measuring device, in another mode shape (not the TE012 mode shape discussed in that paragraph in the Brady report), under ambient pressure, may have resulted in a force measurement without a dielectric, but that the measurements with a dielectric still gave greater force/inputPower measurements than without the dielectric, at NASA.
Excited mode is not relevant. EW has observed force generation without a dielectric.

my recollection is that later discussion by Star-Drive at NSF was to the effect that later measurements in another measuring device, in another mode shape (not the TE012 mode shape discussed in that paragraph in the Brady report), under ambient pressure, may have resulted in a force measurement without a dielectric, but that the measurements with a dielectric still gave greater force/inputPower measurements than without the dielectric, at NASA.
Excited mode is not relevant. EW has observed force generation without a dielectric.
my recollection is that later discussion by Star-Drive at NSF was to the effect that later measurements in another measuring device, in another mode shape (not the TE012 mode shape discussed in that paragraph in the Brady report), under ambient pressure, may have resulted in a force measurement without a dielectric, but that the measurements with a dielectric still gave greater force/inputPower measurements than without the dielectric, at NASA.
Excited mode is not relevant. EW has observed force generation without a dielectric.
All of this is relevant, until the EM Drive is better understood, and these issues are clarified:
* measured in another measuring device instead of the torsional pendulum used previously by NASA Eagleworks,
* measured in another mode shape (not the TE012 mode shape discussed in that paragraph in the Brady report),
* measured under ambient pressure, (not in partial vacuum)
* Star-Drive emphasized the word "may" in "may have resulted in a force measurement without a dielectric"
(Statistical considerations are important in assessing the relevance of any experimental measurement being discussed)
* nobody else, other than NASA has published results comparing the use of HDPE and PTFE dielectrics in a truncated cone and without using them. In particular Shawyer used very different dielectrics: stiff inorganic dielectrics rather than compliant extruded polymers
* the measurements with a dielectric at NASA still gave greater force/inputPower measurements than without the dielectric, at NASA.
* the figure of merit for the EM Drive is the force/PowerInput, not just the force
==> the point being, if the force is thrust that can be used for Space Propulsion and not an experimental artifact, is thrust/PowerInput greater with HDPE and PTFE and if so, under what conditions ?

I keep coming up against people st the moment saying it cannot work because it's a closed system.


I keep coming up against people st the moment saying it cannot work because it's a closed system.That's not the case! Most here have an open mind for the possibility that it may work. This hope is the main reason why we are here. Nevertheless due to the available data we have, we have to accept that it may be due to experimental artefacts. Or can you report some new upcoming data?
I keep coming up against people st the moment saying it cannot work because it's a closed system.
...Energy density in the EM drive oscillates at 2 omega, since it is a scalar magnitude. The E, B and S vectors oscillate at omega. So the 2 omega effect is present in the EM Drive too. The effect of energy density on matter is similar to electrostriction. It contracts as the magnitude of energy density increases, but the effect is negligible small I think....Yes, the energy density, and the Maxwell stress, and the Poynting vector are all oscillating at 2 omega where omega is the frequency of the electromagnetic fields. The E field at omega produces an electrostrictive strain (and hence an elastic stress) on the HDPE or the PTFE also at frequency 2 omega.
Both the electromagnetic forces (Maxwell stress and Poynting vector) and the electrostrictive forces are all acting at the same frequency 2 omega.
The electrostrictive force is out of phase with the electromagnetic force (due to tan delta) a very small amount (delta), which does give a small effect
Tan delta
PTFE ("Teflon") 0.00028 @ 3 GHz
HDPE 0.00031 @ 3 GHz
So delta is only 0.016 degrees (1/62 of a degree), 0.018% of 90 degrees
...Energy density in the EM drive oscillates at 2 omega, since it is a scalar magnitude. The E, B and S vectors oscillate at omega. So the 2 omega effect is present in the EM Drive too. The effect of energy density on matter is similar to electrostriction. It contracts as the magnitude of energy density increases, but the effect is negligible small I think....Yes, the energy density, and the Maxwell stress, and the Poynting vector are all oscillating at 2 omega where omega is the frequency of the electromagnetic fields. The E field at omega produces an electrostrictive strain (and hence an elastic stress) on the HDPE or the PTFE also at frequency 2 omega.
Both the electromagnetic forces (Maxwell stress and Poynting vector) and the electrostrictive forces are all acting at the same frequency 2 omega.
The electrostrictive force is out of phase with the electromagnetic force (due to tan delta) a very small amount (delta), which does give a small effect
Tan delta
PTFE ("Teflon") 0.00028 @ 3 GHz
HDPE 0.00031 @ 3 GHz
So delta is only 0.016 degrees (1/62 of a degree), 0.018% of 90 degrees
If my equations are correct, and Q is an effective refractive index, K. Then momentum that moves from low potential to higher potential, will gain momentum due to the increase in Q, and vise versa as the reflection moves back to the lower Q at the back. This change in momentum is a force acting at omega!
...Energy density in the EM drive oscillates at 2 omega, since it is a scalar magnitude. The E, B and S vectors oscillate at omega. So the 2 omega effect is present in the EM Drive too. The effect of energy density on matter is similar to electrostriction. It contracts as the magnitude of energy density increases, but the effect is negligible small I think....Yes, the energy density, and the Maxwell stress, and the Poynting vector are all oscillating at 2 omega where omega is the frequency of the electromagnetic fields. The E field at omega produces an electrostrictive strain (and hence an elastic stress) on the HDPE or the PTFE also at frequency 2 omega.
Both the electromagnetic forces (Maxwell stress and Poynting vector) and the electrostrictive forces are all acting at the same frequency 2 omega.
The electrostrictive force is out of phase with the electromagnetic force (due to tan delta) a very small amount (delta), which does give a small effect
Tan delta
PTFE ("Teflon") 0.00028 @ 3 GHz
HDPE 0.00031 @ 3 GHz
So delta is only 0.016 degrees (1/62 of a degree), 0.018% of 90 degrees
If my equations are correct, and Q is an effective refractive index, K. Then momentum that moves from low potential to higher potential, will gain momentum due to the increase in Q, and vise versa as the reflection moves back to the lower Q at the back. This change in momentum is a force acting at omega!
Can you show that with more detail?
Electromagnetic momentum is given by Poynting vector which goes like 2*omega because it is a quadratic function of the fields.
Ditto in General Relativity with the stress-energy-momentum tensor: the momentum density and the momentum flux are a function of the square of the fields:
How come your momentum is a linear function of the fields instead of the square of the fields?
...Energy density in the EM drive oscillates at 2 omega, since it is a scalar magnitude. The E, B and S vectors oscillate at omega. So the 2 omega effect is present in the EM Drive too. The effect of energy density on matter is similar to electrostriction. It contracts as the magnitude of energy density increases, but the effect is negligible small I think....Yes, the energy density, and the Maxwell stress, and the Poynting vector are all oscillating at 2 omega where omega is the frequency of the electromagnetic fields. The E field at omega produces an electrostrictive strain (and hence an elastic stress) on the HDPE or the PTFE also at frequency 2 omega.
Both the electromagnetic forces (Maxwell stress and Poynting vector) and the electrostrictive forces are all acting at the same frequency 2 omega.
The electrostrictive force is out of phase with the electromagnetic force (due to tan delta) a very small amount (delta), which does give a small effect
Tan delta
PTFE ("Teflon") 0.00028 @ 3 GHz
HDPE 0.00031 @ 3 GHz
So delta is only 0.016 degrees (1/62 of a degree), 0.018% of 90 degrees
If my equations are correct, and Q is an effective refractive index, K. Then momentum that moves from low potential to higher potential, will gain momentum due to the increase in Q, and vise versa as the reflection moves back to the lower Q at the back. This change in momentum is a force acting at omega!
Can you show that with more detail?
Electromagnetic momentum is given by Poynting vector which goes like 2*omega because it is a quadratic function of the fields.
Ditto in General Relativity with the stress-energy-momentum tensor: the momentum density and the momentum flux are a function of the square of the fields:
How come your momentum is a linear function of the fields instead of the square of the fields?
What you say is true in a space where the refractive index is a constant, or where the metric is Minkowski's. In the PV Model E and H fields are unaffected or "invariant" with respect to K transformations. However, D and B are not.
S = E x H => S(K) = E x H
Pd = D x B => Pd(K) = (K*D) x (K*B) = K2Pd
where S is the Poynting vector and Pd is the Momentum density vector. This comes from the fact that,
(c/K)2 = 1/(K*ε0*K*μ0)
In PV, Power and Area are covariant with the speed of light, so S is unaffected by K, but momentum density is strongly affected. Now, replace K with Q and...
Edit: Due to the gradient in the potential Q, the energy is either going up-hill or down-hill, and oscillates at omega. There is no way to full-wave rectify this such that up = down.
...
If my equations are correct, and Q is an effective refractive index, K. Then momentum that moves from low potential to higher potential, will gain momentum due to the increase in Q, and vise versa as the reflection moves back to the lower Q at the back. This change in momentum is a force acting at omega!
Can you show that with more detail?
Electromagnetic momentum is given by Poynting vector which goes like 2*omega because it is a quadratic function of the fields.
Ditto in General Relativity with the stress-energy-momentum tensor: the momentum density and the momentum flux are a function of the square of the fields:
How come your momentum is a linear function of the fields instead of the square of the fields?
What you say is true in a space where the refractive index is a constant, or where the metric is Minkowski's. In the PV Model E and H fields are unaffected or "invariant" with respect to K transformations. However, D and B are not.
S = E x H => S(K) = E x H
Pd = D x B => Pd(K) = (K*D) x (K*B) = K2Pd
where S is the Poynting vector and Pd is the Momentum density vector. This comes from the fact that,
(c/K)2 = 1/(K*ε0*K*μ0)
In PV, Power and Area are covariant with the speed of light, so S is unaffected by K, but momentum density is strongly affected. Now, replace K with Q and...
Edit: Due to the gradient in the potential Q, the energy is either going up-hill or down-hill, and oscillates at omega. There is no way to full-wave rectify this such that up = down.what is a linear function of omega there ?
...
In the attached image, P is momentum density, Q = K is the refractive index AND a Quality factor whose stored energy and dissipation vary within the cavity wrt "r". (This actually makes a lot of sense in terms of the Quantum Gravity of harmonic oscillators.)
...
In the attached image, P is momentum density, Q = K is the refractive index AND a Quality factor whose stored energy and dissipation vary within the cavity wrt "r". (This actually makes a lot of sense in terms of the Quantum Gravity of harmonic oscillators.)But if P is momentum and P is a function of Q2, and Q is a function of omega, then that means that momentum is a function of omega2, instead of a linear function of omega ...
