mertcan said:
@Charles Link I would like to express that I really want to dig valuable things related to magnetization,transformers, leakage flux, surface currents, volume currents of iron core, flux conservations in core... out of a nice book or lecture.Regarding your unique expertise on magnetism could you suggest me a nice book or lecture which also includes nice proofs related to topics I mention above?
My textbook dates from 1950's and i'll post its name if i find it.
Look for a 1940's book ,
/start cynicism/
because they predate "Publish or Perish"
which shifted the purpose of textbooks from teaching undergrads how to do practical work
to
impressing one's academic reviewers with one's vector calculus prowess.
/end cynicism/
mertcan said:
Thanks
@Charles Link, but I would like to see the proof of approximation that the magnetic flux from surface of iron core to air is negligible. I can not imagine that it is negligible because the magnetic field is not very small. Could you help me about that?
Referring back to that long tome i wrote in the old thread
@Charles Link mentioned,
https://www.physicsforums.com/threa...we-apply-the-biot-savart.927681/#post-5979758
...........................
Leakage inductance is present because of flux that doesn't couple both windings..
From the Wiki transformer page:
i just drew in a few loops of leakage flux..
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Thought steps required to accept the premise that MMF and hence leakage flux is small:
...
When there's no secondary current
the only MMF present is from primary magnetizing current
and that MMF
will be small
because it's just Flux/Reluctance( of core)
and that's why in a power transformer magnetizing current is generally considered negligible . It is made by design small compared to rated load current in order to make the transformer efficient.
So leakage flux at no load will be roughly 1/(relative permeability of core) X (flux in the core)
and with relative permeability probably at least several hundred if not several thousand,
leakage flux to slide rule accuracy will be zero .
With more digits it'll round off to maybe as much as 1% of core flux which is still near zero.
So how does MMF ever get large ?
-------------------------------------------------------
Initial Refinement to that thought process
Okay let us add secondary current.
As explained in the tome referenced above,
primary MMF increases because of secondary amp-turns.
Okay,
Leakage flux will increase in same proportion ,
but core flux remains the same as before, (voltage is the same)
so leakage flux becomes a larger fraction of core flux than it was at no load.
and as you stated leakage out into the air is not any longer so small.
Designers can control by how much leakage flux increases with load to give the transformer its desired impedance .
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I had the good fortune back in early 1970's to have a three legged transformer core two feet tall and a Variac.
I wound enough turns on it to support 120 VAC and played for days trying to teach mysef to visualize the magnetic flux.
To that end i took an old solenoid coil perhaps the size of a pill bottle and used it for a flux detector. An open circuited coil will deliver volts
equal proportional to dΦ/dt and when dealing with sine waves you can connect it to a high impedance AC millivoltmeter to make yourself a flux detector.
I wound a primary on one leg of that core so i could excite it to known volts/turn, , squeezed flux around it , shifting flux between the secondary legs by shorting them with just a single turn.
I drove the core into mild saturation by applying too much voltage and watched primary current ammeter peg high, and saw leakage flux increase with my solenoid coil flux detector
That's how I developed my mental model for the magnetic circuit approach . Small wonder it's how i think of magnetics to this day. But i had to see and feel it, probably you are academic enough to do it with thought experiments.
old jim