Interpreting the BH curve obtained experimentally

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The discussion centers on tracing the B-H curve of soft magnetic material using electromagnetic induction, with a focus on understanding unexpected results, such as the appearance of two loops at the end of the curve. Participants inquire about the experimental setup, including the type of core used, the frequency of the input current, and the method of measuring induced voltage. It is suggested that the observed loops may be due to saturation effects or eddy currents in the setup. The importance of using a triangle wave current to visualize magnetic retardation and the effects of frequency on the induced voltage is also highlighted. Overall, the conversation emphasizes troubleshooting and refining the experimental approach to accurately interpret the B-H curve.
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Hi
We attempted to trace the B-H curve of soft magnetic material by using principles of electromagnetic induction. Attached with this is the curve obtained. I am unable to figure out why am I getting the two loops at the end?
Please help
 

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Prerana said:
Hi
We attempted to trace the B-H curve of soft magnetic material by using principles of electromagnetic induction. Attached with this is the curve obtained. I am unable to figure out why am I getting the two loops at the end?
Please help

Welcome to the PF.

Can you post a diagram of your test setup? What exactly are you plotting on the x-y axes of that oscilloscope?
 
Indeed Berkman's questions are immediate response to your question.

My first guess was you're saturating the core
but that's premature. I don't even know if you're using a toroid core or an old iron bolt. :smile:
What is nature of your soft iron core,
What is frequency,
Is excitation current a sinewave,
Can we assume you use some sort of integrator to calculate flux?



very interesting experiment, fellows . Don't quit now !
 
Hi Jim and Berkeman
We are using the principle of Electromagnetic induction to trace the bh curve of the soft magnetic material ( Mu metal) . The test setup consists of a primary and secondary coil..The primary coil is wound on a aluminium rod of square cross section. The input current is controlled through a resistor in series with the primary coil and the frequency of input current is 50 Hz. The hysteresis material on which the secondary coil is wound is placed in the solenoid. The hysteresis material is in the form of rod having circular cross section of length of 1.1mm x 80 mm. The emf induced in the secondary coil is given to the power amplifier and then to the integrator. The integrator output is plotted on the Y axis and the input current given to the primary coil is plotted on the X axis of the CRO.
@ Jim and Berkeman:
Does the frequency of the input current affect my hysteresis parameters?
How do I conclude that my material has reached saturation?
Thank you for the quick response!
 

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Well what an interesting setup you have there !

That trace attached to your new post has no loops on end - what is it? Your setup with core not inserted perhaps? Or did you solve the mystery already?

The emf induced in the secondary coil is given to the power amplifier and then to the integrator.

(I assume your amplifier has high input impedance so there's not much current in sense coil compared to excitation coil.)
Since your excitation is sinewave, set your 'scope for ordinary time display and observe current & induced voltage as you slide the core into the solenoid.
Then take a look at input and output of "power amplifier" .
As core is inserted the induced signal gets much larger and we should look to see if we are overdriving that amplifier... if output sinewave peaks flatten out you are saturating the amplifier. You shouldn't be able to saturate an iron rod since so much of the magnetic path is through air.

NEXT -------------------------------

Think about what's going on inside that iron...

With an ideal inductor current and flux would be in phase and your test would show a straight line on your oscilloscope. That's what you'll get with air core and that's almost what the more recent trace looks like...

With real inductor you have hysteresis so expect a B-H loop.

Inside real iron you also have eddy currents which retard the flux because of Lenz's law.
Recall Gauss' h(dot)dl = ienclosed counts ALL the current, not just what current you applied. If you use a voltage sensing coil to measure flux, even the current flowing in it counts.

Your 'scope trace on second post shows a small loop - if it's not your successful B-H loop, then perhaps it's just a little phase shift from eddy currents in your aluminum coil form or imperfect integration, or perhaps even an iron leg brace on bottom of work table underneath your solenoid. So take a look at table's underside..
Also note the aluminum coil form constitutes one shorted turn, if that turns out problematic maybe you can find some square plastic or use balsawood??

How do I conclude that my material has reached saturation?
i doubt you could saturate it but-
use 'scope to observe current and induced voltage vs time as you increase current . As you approach saturation, voltage will depart from a sine shape and i think get "spikey".

If you have a function generator and power amplifier that could drive current, , try this:
I've done it myself and it is a real eye-opener.

drive your setup with a triangle wave current instead of a sinewave and look at induced voltage.
A triangle wave current should give a square wave voltage and you'll see effect of "magnetic retardation" by eddy currents as rounded shoulders on your square wave.

You will see effect of frequency as dramatic rounding of the square wave's edges as frequency increases.

If i can find my old 'scope photos i'll photocopy and attempt to post them.
 
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