Mutal inductance depending on current

Click For Summary
SUMMARY

The experiment demonstrated that mutual inductance increased from 94 mH at 5 mA to 160 mH at 10 mA when using two coils wrapped around a ferromagnetic core at a frequency of 50 Hz. This phenomenon is attributed to the nonlinearity of hysteresis in the material, where the permeability changes with increasing current. The measurements were consistent across multiple trials, confirming the theoretical predictions outlined in the accompanying research paper. The relationship between magnetic field strength (H) and magnetic flux density (B) was crucial in understanding the observed changes in mutual inductance.

PREREQUISITES
  • Understanding of mutual inductance and its calculation
  • Familiarity with hysteresis and magnetic permeability
  • Knowledge of B-H curves for ferromagnetic materials
  • Basic principles of electromagnetism and circuit analysis
NEXT STEPS
  • Study the principles of mutual inductance in electromagnetic systems
  • Learn about hysteresis and its impact on magnetic materials
  • Examine B-H curves for various ferromagnetic materials, particularly silicon-steel laminates
  • Explore circuit design and measurement techniques for inductive components
USEFUL FOR

Electrical engineers, physicists, and students studying electromagnetism, particularly those interested in the behavior of inductive components in circuits.

debelino
Messages
10
Reaction score
1
Homework Statement
Why is mutal inductance rising with the rise of current?
Relevant Equations
M=N2*Ф12/I1
My frient had an experiment in lab. They measured the mutal inductance on two coils wraped around one feromagnetic core.
When the current of the first coil was 1, 2, 3, 4, 5 mA the mutal inductance was 94 mH. Then they were told to rise the current to 10 mA, the mutal inductance went to 160 mH. The frequency was 50 Hz all the time.
Why did the mutal inductance rise?
 
Physics news on Phys.org
Sounds like an error. Can you post the full circuit that was used in the experiment, and details of the test equipment used?
 
It is not an error. Everyone got the same results. In the paper explaining the experiment they said it would happen and asked a question why? The secondary coil was open. They measured the voltage on it and calculated the mutal inductance. My only guess is it happened because of the hysteresis nonlinearity. For small currents the permeability is modeled as one number, but as the current grows the dependence of B and H changes and another, bigger number is required to model the B and H dependance. The higher harmonics are not so visible because of the big inductances.
Is this possible? I am only familiar with electromagnetism in theory...
 
berkeman said:
Can you post the full circuit that was used in the experiment, and details of the test equipment used?
 
If we'll neglect the leakage magnetic flux L=B*SteelArea/I B/I=K*B/H
L5mA/L10mA =B10/B20
From magnetic curve B=f(H) of an usual silicon-steel laminate for transformers: H=magnetic field[magnetizing force] B=magnetic flux density[or induction]
If H=10A/cm B=0.9Wb/m^2
If H=20A/cm B=1.5 Wb/m^2
The ratio 1.5/.9[Wb/m^2]≈160/97 [H]
 
I'm sorry. Wrong part of the B_H curves. For small H [less than 3 A/cm] the B-H curve is parallel with abscise. Let’s say for 5mA supply current H= 1.6 A/cm and for 10mA[ 2 times]= 3.2 A/cm. According to attached curve for 1.6 A/cm B=0.075 Wb/m^2 then μ=0.075/1.6=0.046875 and for 3.2 A/cm B=0.25 Wb/m^2 μ=0.25/3.2=0.078125
L=K*μ
L10mA/L5mA=μ3.2/μ1.6A/cm=0.078125/0.046875≈160/97
244434
 

Attachments

  • B_H Magnetic Curves.jpg
    B_H Magnetic Curves.jpg
    111.5 KB · Views: 301
Is this a steel power transformer thing? I've never noticed any small signal distortion in my ferrite communication transformers...
 
I think the above B-H curve is for low carbon steel and not for silicon-steel laminate[my mistake!].In the book these curve lines are similar.
Here attached it is another B-H curve for Low Carbon Steel as per
https://magweb.us/free-bh-curves/
 

Attachments

  • B_H Low Carbon Steel.jpg
    B_H Low Carbon Steel.jpg
    32.3 KB · Views: 325
M = ## N_2 \phi_{21}/i_1 ## assuming zero secondary current. ## \phi_{21} ## = flux thru secondary due to primary current ## i_1 ##.
so it's essentially dB/dH since H ∝ ## i_1 ##.
B vs. H in your last diagram clearly shows dB/dH starting out low, then rising to a max., then receding again.
So as you increase current, flux will be lower at first, then rise, then drop. You seem to have operated in the lower→higher region.
 

Similar threads

  • · Replies 22 ·
Replies
22
Views
3K
  • · Replies 4 ·
Replies
4
Views
2K
  • · Replies 60 ·
3
Replies
60
Views
7K
  • · Replies 2 ·
Replies
2
Views
3K
Replies
10
Views
3K
  • · Replies 9 ·
Replies
9
Views
2K
  • · Replies 2 ·
Replies
2
Views
3K
  • · Replies 1 ·
Replies
1
Views
2K
Replies
10
Views
3K
  • · Replies 3 ·
Replies
3
Views
2K