Finite-difference time-___domain method: Difference between revisions

Revision as of 16:27, 18 October 2005

Revision as of 09:35, 25 October 2005

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Every modeling technique has strengths and weaknesses, and the FDTD method is no different.

FDTD is a versatile modeling technique used to solve Maxwell's equations. It is intuitive, so users can easily understand how to use it and know what to expect from a given model.

FDTD is a time ___domain technique, and when a [[broad-band]] pulse (such as a [[Gaussian pulse]]) is used as the source, then the response of the system over a wide range of frequencies can be obtained with a single simulation. This is useful in applications where resonant frequencies are not exactly known, or anytime that a broadband result is desired.

Since FDTD is a time-___domain technique which findscalculates the E/ and H fields everywhere in the computational ___domain as they evolve in time, it lends itself to providing animated displays of the electromagnetic field movement through the model. This type of display is useful in understanding what is going on in the model, and to help ensure that the model is working correctly.

The FDTD technique allows the user to specify the material at all points within the computational ___domain. All materials are possible and dielectrics, magnetic materials, etc. can be simply modeled without the need to resort to work arounds or tricks to model these materials.

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FDTD allows the effects of apertures to be determined directly. Shielding effects can be found, and the fields both inside and outside a structure can be found directly.

FDTD providesuses the E and H fields directly. Since most EMI/EMC modeling applications are interested in the E/ and H fields, it is bestconvenient that no conversions must be made after the simulation has run to get these values.

== What are the weaknesses of the FDTD Technique?==