Originally posted by T-rex
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The dielectric (the electric field) is a representation of movements of the aether.
The first order movement, steady state flow, is very tightly coupled to gravity. According to Stowe, gravity = Grad E, the gradient of the Electric field. The gradient of the dielectric.
The second order movement are longitudinal dielectric waves.
The third order movement involves rotation. The magnetic field.
The fourth order movement involves rotating electromagnetic waves across the surface of a conductor. The true transverse electromagnetic wave, that like Schumann waves, travel at the boundary of two different media: the metal and the air, or, when in free space, between the metal and the aether. This is what is known as the near-field in antenna's.
The fifth order movement involves vortexes, in such a way that a phenomenon known as "particles" takes place. This is what is known as the far-field in antenna's.
All right.
Now the interesting thing is that with the longitudinal wave, we have no conjugate pair of L anc C.
L represents the magnetic propagation properties of the medium, which represent the properties of the medium in terms of rotational movements in/of the aether. Since with LD waves, we have no magnetic component, we therefore also should not model the magnetic component to be present. In other words: for the LD mode, we have to take L = 0.
So, for the propagation of the longitudinal dielectric wave, you would have to calculate with C and R, the real part of characteristic impedance of the medium.
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