Example Problem - Toroid: Difference between revisions

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<math>r_m=(\frac{1}{2})\frac{OD + ID}{2} = 2.25\ cm</math>
<math>r_m=(\frac{1}{2})\frac{OD + ID}{2} = 2.25\ cm</math>


Using the mean radius the mean path of length l_m can be calculated.
Using the mean radius the mean path of length <math>l_m</math> can be calculated.




Line 30: Line 30:
<math>H_m=\frac{20 x 2.5}{.141}= 354.6\ A /m)</math>
<math>H_m=\frac{20 x 2.5}{.141}= 354.6\ A /m)</math>


Since the width of the toroid is much smaller than the mean radius r_m we can assume a uniform H_m throughout teh cross-section of the toroid.
Since the width of the toroid is much smaller than the mean radius <math>r_m</math> we can assume a uniform <math>H_m</math> throughout teh cross-section of the toroid.

Revision as of 11:58, 19 January 2010

Problem: Concerning Ampere's law Let look at a coil around a toroid shown in the figure below. The coil has N = 20 turns around the toroid. The toroid has an inside diameter of ID = 4 cm and an outside diameter OD = 5 cm. Determine the field intensity H along the mean path length within the toroid with a current i = 2.5 A.

Toroid.jpg


Figure created by Kirk Betz


Solution:

Do symmetry the magnetic field intensity Hm along a circular contour within the toroid is constant. We can find the mean radius by


Using the mean radius the mean path of length can be calculated.


With Ampere's Law (below) the field intensity along the mean path can be Found.

Finally teh H_m can be calculated.

Since the width of the toroid is much smaller than the mean radius we can assume a uniform throughout teh cross-section of the toroid.