Hi Exnihiloest,
The answer is in the geometry and the permeability of the two materials i.e. air and ferromagnetic core.
Because the flux is conserved, there must be a value of flux outside the solenoid that exactly matches the value inside the solenoid - A one to one match for every line of flux.
However, the occupied space of those values is radically different, therefore we are discussing the concentration within a given volume, not the total quantity.
The inside area is a finite space.
The outside area is confined only by the boundaries of the universe (if such exist) and is therefore considered infinite.
So, depending on the thickness and permeability of your exterior core, only a small fraction of the actual exterior flux is routed through that material. Of course it is possible to find a value of permeability and thickness that could contain all (or nearly so) of the exterior flux and then the two experiments would be nearly identical.
The formulae for determining inductance is as varied as the geometry: http://en.wikipedia.org/wiki/Inductor#Inductance_formulae
Hi Harvey,
I well understand your reply and I think it is the likely explanation which is qualitatively in perfect agreement with the laws of electromagnetism. Nevertheless I would like to check it quantitatively because a question remains.
If there is no magnetic material and we chose a particular surface outside of the coil, we have some flux crossing it. If the air is replaced by a material of high magnetic permeability, the flux through the same area will be strongly increased. This is traditionally represented by field lines curving towards the magnetic material, resulting in more lines crossing the same area. It is the principle used in a ferrite rod AM antenna: for the same flux, the crossed section in air is much wider than in the rod, and this allows the antenna to work as if its geometrical dimensions were 10 to 30 times larger.
Small ferrite rod antennae have replaced old big loop. Same effet for this:
And this:
We all have a mental image of the field lines of a coil, extending until infinity all over the space around from one end of the coil to the other one. But if we replace air outside of the coil with a magnetic material, the image has to be modified: the presence of the material changes the space properties around the coil and the magnetic flux preferably follows the sections of higher permeability (consequence of the principle of least action). And so when the permeability of a surrounding medium is not uniform, we have not at all the same flux crossing the same arbitrary area, we have much more flux through to the sections of higher permeability that bend the field lines. Your reply shows clearly that you know that, but this point must emphasized. The quantity of flux must be calculated otherwise it is not concluding:
The infinity of the space around a coil is not a sufficient reason to suppose that the most of magnetic flux would not take the ferrite path."The magnetic field is concentrated through the ferrite rod"
I’m aware that inside the coil, the cross section is the same either with air or with a magnetic material, and of course we cannot expect for the same effect outside of the coil even though an external magnetic material attracts the flux.
But I wonder why ferrite outside of a coil that is completely embedded in it, changes the resonant frequency by
only 7% while we would be expecting for much more because of the ability of the high permeability material to “suck” the magnetic flux at the detriment of the flux in air. Although the change of the coil inductance is more than 7% because it is the resonant frequency square that is proportional to the inductance, it is not much and it is considerably much less than with the ferrite inside the coil.
The difference of the effect between ferrite inside and outside is not astonishing but the order of magnitude of the difference is. It puzzles me and motivates for further tests.
My first test has flaws:
- There is a 2mm gap between the external circumference of the ferrite cylinder and the outside coil
- There is a 1mm gap between the internal circumference of the ferrite cylinder and the inside coil
- The inside coil is thick with several layers of turns, and so it has a not constant diameter, while the outside coil is thin
I will wound a wire directly outside and inside the ferrite cylinder, without gap, and see what will be going on.
But one important aspect relates to the formula Φ = BA = µNπr²i / ℓ where the total flux (Φ) is shown to increase if either the flux density (B) or the area (A) are increased as it is the product of the two. And since the flux density is dependent on the relative permeability of the interior core (µ) in the formula B = µNi / ℓ we expect more flux when there is higher permeability in the core e.g. ferromagnetic core vs air. Alternatively, we could write it as B = Φ/A
So the middle of the solenoid is a finite area that we can use in our calculations. But once we leave that defined volume these formulas become difficult as A would represent the universe (or at least a measurable volume magnitudes larger than the solenoid center) and we are looking for a cross sectional area where the flux is normal to it.
Hope that helps
I agree with these formulae and the difficulty of real calculus for any area, anywhere, and with any permeability. This is the question to be experimentally verified. The flux being supposed conservative, the same action upon a section of same flux should not depend on the location of the section that we deal with, whether it is inside or outside.