How Can a Toroid Approximate a Solenoid in Limiting Conditions?

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SUMMARY

The discussion focuses on the mathematical relationship between the magnetic fields of solenoids and toroids, specifically under limiting conditions. Chris W presents the equations for both configurations: B = μo i n for solenoids and B = (μo i N) / (2Π r) for toroids, where N represents the total number of turns. The key conclusion is that as the difference between the inner and outer radii of the toroid approaches zero, the toroid's magnetic field can be approximated to that of a solenoid over a small length L. This relationship is established through the application of limits.

PREREQUISITES
  • Understanding of magnetic field equations, specifically B = μo i n and B = (μo i N) / (2Π r)
  • Familiarity with the concept of limits in calculus
  • Knowledge of the physical properties of solenoids and toroids
  • Basic understanding of Ampere's law and magnetic field calculations
NEXT STEPS
  • Study the derivation of magnetic fields in solenoids and toroids
  • Learn about the application of limits in calculus, particularly in physics
  • Explore the relationship between total turns and turns per unit length in magnetic field equations
  • Investigate practical applications of solenoids and toroids in electromagnetic devices
USEFUL FOR

Physics students, electrical engineers, and anyone interested in the principles of electromagnetism and magnetic field theory.

Chris W
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Hi everyone.
I need help please.
I am working on problems with solenoids and Toroids
I have solution for the solenoid:
B = μo i n

And toroid:
B = (μ o i n)/ (2Π r)
Also, I know that the magnetic field is the function of r namely: B = B(r)

r- radius of the Ampere’s path
n – number of loops per unit length
i-Current
μo – constant

My problem is:
Using the solution for the toroid, show that for the large toroid the answer can be approximated as the solenoid on the very small piece of the toroid.
I know that I have to play with limits. Something like:
a - inner radius of the toroid,
b – outer radius of the toroid,
∆a - the difference between radius a and radius b.
I think I have to take a limit when ∆a goes to 0 and in this way radius a will approach radius b. in this way the solution for the toroid SHOULD be the solution for the solenoid (on the small length L of course)
I don’t know how to set it up. How to get from the toroid solution to the solenoid solution using limits or (other technique)

Thanks for help
Chris W
 
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Can anyone please help me here... thanks
Chris W
 
Hi Chris W,

Your toroid magnetic field equation is not quite right. It should be:

<br /> B = \frac{\mu_0 i N }{2\pi r}<br />

where N is the total number of turns (not turns per length). Notice that N/(2 \pi r) is in a way similar to the n in the solenoid formula; but what is the difference? If you then think about your limiting process that should help you get the result.
 
Thanks Guys. I love this forum
!
Chris W
 

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