Example: Magnetic flux density inside an infinitely long solenoid (a) As a direct application of Ampère's circuital law B field must be parallel to the axis (Why?) No magnetic field outside (Why?) -

Principles of Physics: A Calculus-Based Text
5th Edition
ISBN:9781133104261
Author:Raymond A. Serway, John W. Jewett
Publisher:Raymond A. Serway, John W. Jewett
Chapter23: Faraday’s Law And Inductance
Section: Chapter Questions
Problem 48P
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1. The reason that B field must be parrallel

2. The reason there should be no magnetic field outside

●
Example: Magnetic flux density inside an infinitely long solenoid
(a) As a direct application of Ampère's circuital law
B field must be parallel to the axis (Why?)
- No magnetic field outside (Why?)
BL=μ₂nLI ⇒ B = μ₂nI
(n: number of wound turns per unit length)
-
(b) As a special case of toroid
N
B = H₂
2πb
I = μ₂nl
Transcribed Image Text:● Example: Magnetic flux density inside an infinitely long solenoid (a) As a direct application of Ampère's circuital law B field must be parallel to the axis (Why?) - No magnetic field outside (Why?) BL=μ₂nLI ⇒ B = μ₂nI (n: number of wound turns per unit length) - (b) As a special case of toroid N B = H₂ 2πb I = μ₂nl
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