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   [1D] FDTD
  electromagnetic wave simulations of propagating waves in non-magnetic and
  lossy dielectric media  Ian Cooper Please
  email any corrections, comments, suggestions or additions  matlabvisualphysics@gmail.com View  ELECTROMAGNETISM USING THE FDTD METHOD ft_03.m Download and run the script ft_03 .m. Carefully inspect the script to see how the FDTD method is implemented. Many variables can be changed throughout the script, for example, type of excitation signal, boundary conditions, time scales, properties of the medium. We can also model the propagation of EM waves in materials where the loss term is specified by the conductivity of the material. This loss term results in the attenuation of the propagating energy. A wave encountering a boundary between media with different refractive indices (relative permittivities) will in general be partially refracted (transmitted) and partially reflected at the boundary. The relationship between the incident wave and the refracted and reflected waves can be expressed in terms of the transmission T and reflection R coefficients. This relationship can be expressed in terms of impedances Z or refractive indices n. For a
  non-magnetic and non-lossy dielectric medium, the speed of propagation c
  of an electromagnetic wave depends on the refraction index n of
  the medium. The refractive index n is a function of
  the relative permittivity               
   For an
  electromagnetic wave the impedance Z is defined as the
  ratio between the magnitudes of the E and H
  fields. For a medium with dielectric constant           
                     
   The
  impedance of free space is   For our [1D] model of the incident wave reaching the boundary, we must have         and         In the
  case of non-magnetic material                   The amplitude for the electric field propagating in the +Z direction in a lossy dielectric medium is given by         The two parameters and are given by               
 Simulations Parameters: Nt = 1000 Nz = 300 lambda = 3x108/(400x106) (f = 400 MHz) eR1 = 1 S = 0 S2 = 0.01 zS = 150 
 Fig. 1. Animation of sinusoidal EM wave striking a lossy dielectric medium 
 Fig. 2. Probes measurements of electric field. 
 Fig. 3. Figure Window summary of results. There is reasonable agreement between the theoretical predictions and the values calculated from the exponential decay of the EM wave in the lossy dielectric medium.  |