Ferrite core variable inductor

AI Thread Summary
The discussion focuses on designing a variable inductor using a ferrite core, where increasing DC current through a main winding decreases the inductance on a side arm due to reduced permeability. The designer seeks to understand the physical reasons behind this phenomenon and the inherent inaccuracies in their measurements, which show significant variance. Concerns are raised about the non-linear and imprecise nature of using core saturation for inductance control, especially given the need for precise adjustments in the application of simulating vehicle detection in inductive loops. The specifications indicate a required inductance range of 50-750 µH with rapid electronic adjustments, but the current design struggles with repeatability and accuracy. The conversation highlights the complexities of core physics and the challenges in achieving desired precision in variable inductors.
jrand26
Messages
11
Reaction score
0
Hi all, I'm working on designing a variable inductor using a ferrite core. The basic idea is that I have a large wound inductor on the central arm which I pass a DC-current through, and a smaller, variable inductor on one of the side arms. As you increase the current through the main winding, the inductance on the side arm decreases. Am I correct in saying that this is due to a drop in permeability in the core? As per the equation,

L = \frac{\mu N^2 A}{l}
What is the physical explanation for an increased current causing a decrease in permeability in the core? Image 1 shows something similar, except I'm only using one of the side arms and there is no air gap on the central winding.

While the design essentially works I'm not satisfied with the accuracy. The biggest problem I've been having is that when I repeat my measurements I get quite a spread of results, which I find really interesting (image 2 shows the curve bounded by max/min measurements). Is there something about the physics of the core which makes it inherently difficult to control? I have noticed hysteresis but I'm not sure that it should effect repeatability. I'm also unsure of the shape of the curve, why does the inductance increase with increasing current briefly at the start?

Any help/comments or links to other resources appreciated :)
 

Attachments

  • image_1.jpg
    image_1.jpg
    21.5 KB · Views: 811
  • image_2.jpg
    image_2.jpg
    18.8 KB · Views: 723
Physics news on Phys.org
jrand26 said:
Hi all, I'm working on designing a variable inductor using a ferrite core. The basic idea is that I have a large wound inductor on the central arm which I pass a DC-current through, and a smaller, variable inductor on one of the side arms. As you increase the current through the main winding, the inductance on the side arm decreases. Am I correct in saying that this is due to a drop in permeability in the core? As per the equation,

L = \frac{\mu N^2 A}{l}
What is the physical explanation for an increased current causing a decrease in permeability in the core? Image 1 shows something similar, except I'm only using one of the side arms and there is no air gap on the central winding.

While the design essentially works I'm not satisfied with the accuracy. The biggest problem I've been having is that when I repeat my measurements I get quite a spread of results, which I find really interesting (image 2 shows the curve bounded by max/min measurements). Is there something about the physics of the core which makes it inherently difficult to control? I have noticed hysteresis but I'm not sure that it should effect repeatability. I'm also unsure of the shape of the curve, why does the inductance increase with increasing current briefly at the start?

Any help/comments or links to other resources appreciated :)

It looks like you are wanting to use saturation of the core to reduce the effective inductance. This is not a very precise or linear way to accomplish this. Is there a reason you are wanting to control the inductance this way? What is the context of this circuit, and what is the application?
 
berkeman said:
It looks like you are wanting to use saturation of the core to reduce the effective inductance. This is not a very precise or linear way to accomplish this. Is there a reason you are wanting to control the inductance this way? What is the context of this circuit, and what is the application?

I'm an EE student doing vac-work at a place where they essentially want a variable inductor, but controllable to really precise levels (up to 0.01 mu H). Someone here before me did their thesis on methods for doing this and they determined that this was the best solution, and my project here is to continue on from there.

It seems like a pretty cool solution to the problem, but I can't really say it's that precise if it has such variance in testing. I was thinking by posting the problem here I might get a better understanding of the physics behind the design and the associated limitations.

Would you be able to expand on why this method is imprecise/non-linear? It seems pretty linear to me over a range of current values, although the type of curve doesn't really matter does it? Although I might have misinterpreted what you meant.
 
jrand26 said:
I'm an EE student doing vac-work at a place where they essentially want a variable inductor, but controllable to really precise levels (up to 0.01 mu H). Someone here before me did their thesis on methods for doing this and they determined that this was the best solution, and my project here is to continue on from there.

It seems like a pretty cool solution to the problem, but I can't really say it's that precise if it has such variance in testing. I was thinking by posting the problem here I might get a better understanding of the physics behind the design and the associated limitations.

Would you be able to expand on why this method is imprecise/non-linear? It seems pretty linear to me over a range of current values, although the type of curve doesn't really matter does it? Although I might have misinterpreted what you meant.

Can you post more about the specifications for this variable inductor? What range of inductances are needed? What is the amplitude of the AC signal that needs to "see" this inductance, compared to the range of DC saturating current that you are using? How quickly do you need to change the inductance? (Like, could you just use a moving slug variable inductor, or do you need to be able to adjust the inductance elecronically fairly rapidly?)

What is the application of this variable inductor? Can it be implemented with a gyrator circuit instead?
 
berkeman said:
Can you post more about the specifications for this variable inductor? What range of inductances are needed? What is the amplitude of the AC signal that needs to "see" this inductance, compared to the range of DC saturating current that you are using? How quickly do you need to change the inductance? (Like, could you just use a moving slug variable inductor, or do you need to be able to adjust the inductance elecronically fairly rapidly?)

What is the application of this variable inductor? Can it be implemented with a gyrator circuit instead?

Range is about 50-750 mu H, application is in simulating vehicle passing over in-ground inductive loops. I'm not aware of any restrictions on the AC signal or DC saturating current. It needs to change quickly electronically (I'm doing that with a DAC).

A gyrator circuit was looked at but would require a digital potentiometer with higher resolution than is available.
 
This is from Griffiths' Electrodynamics, 3rd edition, page 352. I am trying to calculate the divergence of the Maxwell stress tensor. The tensor is given as ##T_{ij} =\epsilon_0 (E_iE_j-\frac 1 2 \delta_{ij} E^2)+\frac 1 {\mu_0}(B_iB_j-\frac 1 2 \delta_{ij} B^2)##. To make things easier, I just want to focus on the part with the electrical field, i.e. I want to find the divergence of ##E_{ij}=E_iE_j-\frac 1 2 \delta_{ij}E^2##. In matrix form, this tensor should look like this...
Thread 'Applying the Gauss (1835) formula for force between 2 parallel DC currents'
Please can anyone either:- (1) point me to a derivation of the perpendicular force (Fy) between two very long parallel wires carrying steady currents utilising the formula of Gauss for the force F along the line r between 2 charges? Or alternatively (2) point out where I have gone wrong in my method? I am having problems with calculating the direction and magnitude of the force as expected from modern (Biot-Savart-Maxwell-Lorentz) formula. Here is my method and results so far:- This...
Back
Top