Show that for a ferromagnetic material the field in the gap is given by?

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Homework Help Overview

The problem involves a toroidal magnetic material with a gap, where participants are tasked with showing how the magnetic field in the gap can be expressed in terms of the number of loops, current, and gap length. The subject area is magnetism, specifically focusing on ferromagnetic materials and magnetic fields.

Discussion Character

  • Exploratory, Conceptual clarification, Mathematical reasoning

Approaches and Questions Raised

  • The original poster attempts to derive the magnetic field in the gap using assumptions about uniformity and parallelism of magnetic quantities. Some participants question the consistency of the derived expressions for magnetic intensity H in different contexts, suggesting a need for clarification on the relationship between magnetomotive force and magnetic intensity.

Discussion Status

The discussion is ongoing, with participants exploring different interpretations of the magnetic intensity and its implications for the problem. Some guidance has been offered regarding the definitions and relationships between terms, but no consensus has been reached yet.

Contextual Notes

Participants are navigating potential assumptions about the uniformity of the magnetic field and the implications of the gap in the toroidal structure. There is also a discussion on the definitions of magnetomotive force and its role in the calculations.

blueyellow

Homework Statement



A toroidal shaped magnetic material of radius, a, and cross sectional radius R has a small transverse gap cut into it of length l. The toroid is uniformly overwound with a coil of N loops carrying a current I. Show that for a ferromagnetic material the field in the gap is given by

B~mu0 N I/l

[5 marks]

The Attempt at a Solution



Assume that the curvature is small, so that locally B, H and M are parallel to each other, uniform across the cross-section and tangential. A circular loop integral of radius R will have the same value of H at every point, so:

the loop integral of H.dl=H 2 pi R=NI

H=NI/2 piR

2 pi R is the circumference, so for a toroid with a gap of length l:

H=NI/l

B=mu0(H+M)

M=0 because the gap is made of empty space

B=mu0 (H+0)

=mu0 NI/l

Have I gone wrong somewhere by saying something that's not true? I'd be grateful if you could help please.
 
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If H = Ni/2piR, then it's kind of hard to believe that H = Ni/l, isn't it?

Hint: what is Ni, which is magnetomotive force, in terms of H(gap), H(material), l and R?
 
NI is the magneetic force? The number of turns on the toroid multiplied by the current is the magnetic force?
 
blueyellow said:
NI is the magneetic force? The number of turns on the toroid multiplied by the current is the magnetic force?

I know it by "magnetomotive" force, mmf. It's the magnetic equivalent of electromotive force in electricity.

In electricity, it's emf = -N*∂φ/∂t = iR = El, i = current, R = resistance, φ = magnetic flux, N = no. of turns, R = l/σA, A = area, σ = conductivity, l = path length, E = electric field.

In magnetics, it's mmf = Ni = φR' = Hl, R' = magnetic reluctance, H = magnetic intensity, R' = l/μA, μ = permeability, B = μH.
 
Last edited:

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