Well, I did say steel. Ok fine, AISI 1020 steel, as sand-cast. What more do you need to know?
As for hole, let's say 12mm ID, and wire to make 50 ohm coax. Wire is copper, C110 alloy half-hard let's say. The copper might be held centered with a solid, foam or spider structure thingy of whatever material; if you insist, let's say it's foamed polyethylene.
I will provide you with a reference to a book about electromagnetic shield design for aerospace equipment, where you can find some straightforward formulas for estimation. It explains shield estimation with an example that is very close to your question, with just one exception - without a hole with wire.
Say we attach the receiver at the surface of the cube. Wire does not extend beyond the cube. Is there still a leakage path?
Technically, you described a classic GP antenna and asked whether there will be radiation leakage from it. Yes it has radiation loss.
But now you proposed to connect the ground of the remote receiver with a wire to the ground plane of the transmitter antenna and are asking if it will still be able to radiate. Yes, it will radiate. Why not?
I just wonder why you decided that the wire between transmitter and receiver ground will block the transmission?
Ok, that's incorrect. You require further study on this point.
What exactly incorrect and why?
If you claiming that the cube surface is not involved in radiation process, then this is nonsense.
The surface of the metal cube acts as a counterpoise to the antenna's radiator (the part of wire outside cube).
The hole with wire works here as coax cable to deliver RF energy from oscillator inside cube to the cube surface.
At the cube's surface, it feeds a GP antenna, where the radiator is the part of the wire outside the cube and the counterpoise is the cube's outer surface (ground plane).
Do I understand correctly that you are claiming the GP antenna fed from the oscillator with coax cable will not radiate?
There are no reflections, the material is wholly absorptive (skin effect dominant) and fields decrease exponentially with depth into the material.
This is your mistake. There is no material in the world that absorbs all energy of electromagnetic wave that penetrate into it.
You can find correction for wave reflections inside metal shield plate in literature about electromagnetic shield design for aerospace equipment.
A little bit later I will give you the reference on a book which explains it in details with math.
Attenuation will be exceptional, even at fractional Hz. It seems further study in this direction is also warranted.
Even if you use some meta-material with exceptional attenuation, it still just attenuate electromagnetic wave, but not cancel it to zero.
And as I remember my calculations, 0.5 meters metal plate has pretty bad attenuation for magnetic field at low frequencies even above 1 Hz.
By extension, as the block is solid and conductive, near electric field is zero by definition.
by definition? by whose definition?
Do I understand correctly that you are claiming it's impossible to radiate an electromagnetic wave with an antenna made from conductive material?
Sorry, but in this case, you are saying things that are complete nonsense.
The conductor can
attenuate electromagnetic wave very high but
not cancel it to zero.
Therefore, for a good shielding, it is necessary to use a sufficiently thick shield plates.
The intensity of the electromagnetic wave decreases as it penetrates deeper into the conductor. However, if you understand the nature of the skin-effect, you know very well that complete cancel of the electromagnetic wave does not occur even if you increase the size of the shielding cube’s wall to enormous dimensions.
The majority part of the current induced in the conductor will flow near the surface, but that doesn’t mean the electromagnetic wave won’t induce currents deeper within the conductor. It will induce currents deeper than skin-layer, but they will be much smaller than close to surface. How much depends on the frequency and conductor properties. The skin depth simply indicates the thickness of the surface layer where the majority of the current flows, but
not all of the current induced by the electromagnetic wave.
If electromagnetic waves could not exist inside a conductor, then electromagnetic waves would not be able to induce currents in the conductor at all, and the concept of skin-effect depth would lose all meaning.
Hmm interesting. If I carve off the corners to make a maximally sized octahedron let's say, what parameters change, and by how much? Surely you have a quantitative value in mind...
It's hard to predict the near-field configuration for a custom-shaped antenna. I don’t think there is a simple rule for that. So, if you want to know how changes in antenna shape affect its near field configuration, radiation efficiency and radiation pattern, it’s better to use an electromagnetic simulator.
I think for a GP with ground plane shaped as a cube or octahedron, you can use even some
NEC-model based simulator. It uses simplified simulation, but I think it will be well enough for your case.