Attenuation of a Sinusoidal Magnetic Field in a Halfspace Conductor

Requires a Wolfram Notebook System

Interact on desktop, mobile and cloud with the free Wolfram CDF Player or other Wolfram Language products.

Requires a Wolfram Notebook System

Edit on desktop, mobile and cloud with any Wolfram Language product.

When a block of conductor is subjected to a changing magnetic field, a current is induced inside the conductor. This Demonstration shows this phenomenon when a sinusoidal magnetic field is applied to a halfspace conductor. The magnetic field of moderate frequency (and therefore, regarded as a near field) is assumed to be parallel to the conductor surface. The skin depth is determined by the frequency as well as the conductor parameters of conductivity and relative permeance . Taking the direction of the magnetic field as the -axis, the current is directed along the -axis. The spatial distributions of and (to which the electric field is proportional: ) are shown graphically.

[more]

You can choose copper, iron, or brine (sea water) as the conducting medium. The amplitude of the exciting magnetic field is fixed at 1 A/m, but the frequency and the observation time (or phase) are variable. You can see an animation of the spatial distribution by changing the observation time.

[less]

Contributed by: Y. Shibuya (November 2012)
Open content licensed under CC BY-NC-SA


Snapshots


Details

Snapshot 1: the skin depth of copper is about 200 μm in a 0.1 MHz field

Snapshot 2: the high permeance of iron contributes to decreasing the diffusing distance

Snapshot 3: brine, a poor conductor, still retains screening effects to lengths of the order of meters

The electromagnetic fields in a conductor are governed by the diffusion equation, in which the skin depth is given by . The values for copper and iron are much smaller than for brine. The fields, a function of space and time, are expressed as

,

,

.

The maximum values are related by , , , where the amplitude of the applied field is set equal to . Those values are shown in the table at the bottom. For copper and brine, the maximum magnetic field is equal to the applied field (); however, the interior field for iron becomes much smaller due to the large permeance.

As seen from the equations, the field distribution is quite analogous in all cases. The skin depth is the only parameter to define. The distribution curve may suggest a wave propagation into the interior. However, this phenomenon is not the electromagnetic wave defined by Maxwell's equations, but rather the result of diffusion of the magnetic field, which occurs at a variable speed.

Reference

[1] G. Lehner, Electromagnetic Field Theory for Engineers and Physicists (M. Horrer, trans.), New York: Springer, 2009.



Feedback (field required)
Email (field required) Name
Occupation Organization
Note: Your message & contact information may be shared with the author of any specific Demonstration for which you give feedback.
Send