Example: Ampere's Law: Difference between revisions
Jump to navigation
Jump to search
No edit summary |
|||
(3 intermediate revisions by the same user not shown) | |||
Line 10: | Line 10: | ||
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.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> |
||
One can assume a uniform H<sub>m</sub> throughout the cross-section of the toroid because the width is smaller than the mean radius. |
|||
===Author=== |
===Author=== |
Latest revision as of 19:43, 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
The mean path length is
The mean path length encloses the current i N-times.
From Eq. 5-1
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