Example: Ampere's Law: Difference between revisions

From Class Wiki
Jump to navigation Jump to search
Line 11: Line 11:
The mean path length is <math>L_m = 2*\pi*r_m = 2\pi*6.25\approx .393m</math>
The mean path length is <math>L_m = 2*\pi*r_m = 2\pi*6.25\approx .393m</math>


The mean path length encloses the current i N-times.[[Image:toroidish|thumb|widthpx| ]]
The mean path length encloses the current i N-times.[[Image:toroidish.jpg|thumb|widthpx| ]]


From Eq. 5-1 <math>H_m = \frac{N*i}{L_m} = \frac{50*5}{.393}\approx 636</math>
From Eq. 5-1 <math>H_m = \frac{N*i}{L_m} = \frac{50*5}{.393}\approx 636</math>

Revision as of 20:42, 18 January 2010

Problem Statement

Consider a toroid which has N = 50 turns. The toroid has an ID = 10cm and OD = 15cm. For a current i = 5A calculate the field intensity H along the mean path length within the toroid. (this problem is similar to Example 5-1 in the text book)

Solution

The magnetic field intensity Hm is constant along the circular contour because of symmetry.

The mean path length is rm=12*(OD+ID2)

The mean path length is Lm=2*π*rm=2π*6.25.393m

The mean path length encloses the current i N-times.

File:Toroidish.jpg

From Eq. 5-1 Hm=N*iLm=50*5.393636

One can assume a uniform Hm throughout the cross-section of the toroid because the width is smaller than the mean radius.

Author

Tyler Anderson

Reviewers

Readers