Calculate flux in a ferrite bead on a wire

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SUMMARY

The discussion focuses on calculating the magnetic flux in a ferrite bead surrounding a wire carrying a constant current I. According to Ampère's law, the magnetic field component is given by H_{\phi} = I / (2 \pi r). The magnetic flux through the ferrite bead, defined by internal radius a and external radius b, is calculated as Φ = μ₀μᵣ(I / (2π)) ln(b/a). The inductance L is derived from the flux as L = Φ / I. The conversation clarifies the need to consider the axial length of the bead when calculating flux, emphasizing the ferrite's high permeability in determining the overall inductance.

PREREQUISITES
  • Understanding of Ampère's law and magnetic fields
  • Familiarity with magnetic permeability (μ₀ and μᵣ)
  • Basic knowledge of inductance and its calculation
  • Concept of integrating functions in cylindrical coordinates
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  • Study the derivation of magnetic fields in cylindrical coordinates
  • Learn about the properties of ferrite materials and their applications in electronics
  • Explore advanced inductance calculations for complex geometries
  • Investigate the effects of high permeability materials on circuit performance
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Electrical engineers, circuit designers, and anyone involved in the design and analysis of inductive components in electronic circuits.

EmilyRuck
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Suppose that a ferrite bead is put around a cable where a constant current I flows, just like in this image.

The coordinate system has the z axis along the cable. Let's evaluate the current through the (x,y) plane: according to the Ampère's law, the only magnetic field component generated by that current is

H_{\phi} = \displaystyle \frac{I}{2 \pi r}

where r is the distance from the origin.
In order to calculate the inductance of the wire with the ferrite bead, the magnetic flux through the ferrite should be calculated first.
The ferrite bead has a as internal radius and b as external radius, so it is present in the (x,y) plane only for a \leq r \leq b. It surrounds the conductor (which has of course a section diameter less than 2a) and the flux of the magnetic field through the ferrite bead should be:

\Phi = \mu_0 \mu_r \displaystyle \frac{I}{2 \pi} \int_a^b \displaystyle \frac{1}{r} dr = \displaystyle \frac{\mu_0 \mu_r I}{2 \pi} \ln \left( \displaystyle \frac{b}{a} \right)

Then the inductance is L = \Phi / I as usual.

My question is: why is the flux calculated in such a way?? Should not be considered all the surface surrounded by the circuit or something similar? (I know, it is a linear cable and I didn't specify that area)
 
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It makes sense to speak of the inductance of the wire/bead combination because the ferrite has a high permeability so its inductance dominates over that of the rest of the wire. Does that address your question?
 
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Thant means the thickness of the ferrite bead is unity
 
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Thanks to both of you. And for @marcusl yes, sure, your observations address my question.
 
I think there's a small slip. You need to integrate the flux through an area at right angles to the flux, so you need to multiply by the axial length of the bead. Alternatively you must interpret your Phi as flux per unit axial length of bead.
 
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