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1.4 PROPAGATION IN A DIELECTRIC MEDIUM

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In order to simulate a medium with a dielectric constant other than 1, which corresponds to free space, we have to add the relative dielectric constant εr to Maxwell’s equations:

(1.13a)

(1.13b)

We will stay with our one‐dimensional example,

(1.14a)

(1.14b)

then go to the finite‐difference approximations and make the change of variables in Eq. (1.5):

(1.15a)

(1.15b)

From this we can get the computer equations

(1.16a)

(1.16b)


Figure 1.4 Simulation of a pulse striking dielectric material with a dielectric constant of 4. The source originates at cell number 5.

where

(1.17)

over those values of k that specify the dielectric material.

The program fd1d_1_3.py simulates the interaction of a pulse traveling in free space until it strikes a dielectric medium. The medium is specified by the parameter cb in Eq. (1.17). Figure 1.4 shows the result of a simulation with a dielectric medium having a relative dielectric constant of 4. Note that one portion of the pulse propagates into the medium and the other is reflected, in keeping with basic EM theory (6).

Electromagnetic Simulation Using the FDTD Method with Python

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