Truncation boundary for impedance matching layer
An impedance matching and boundary technology, applied in special data processing applications, instruments, electrical digital data processing, etc., can solve problems such as Cartesian coordinate calculation methods that have not yet appeared
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example 1
[0043] Example 1. Solve a two-dimensional problem to verify the setting of the absorption effect of the impedance matching layer. The content of the two-dimensional modeling file is: the calculated area range is (0,0)→(300,300), and the space step is Δ x =Δ y= 0.25cm, the time step is Δ t= 0.41667ps, the entire calculation area is in a vacuum state, and its conductivity is σ =0, the magnetic permeability is mu 0 , the dielectric constant is ε 0 . The point source of the time harmonic field is selected as the excitation source, and the expression is E z =sin(2 πf 0 N Δ t ), f 0 is the frequency of the source, and the number of iterations of the electromagnetic simulation is N =1050. Run the program thus, the result is as follows image 3 shown. When the point source is placed in the center of the calculation area, an obvious concentric circle diagram can be obtained. image 3 (a) and (b) show no reflection of electromagnetic waves. When the eccentric coord...
example 2
[0044] Example 2. Near-field scattering of a two-dimensional infinitely long conducting cylinder. The calculated area range is (0,0)→(250,250), and the space step is Δ x =Δ y= 0.25cm, the time step is Δ t= 0.41667ps, the conductor cylinder is located in the center of the calculation area, and its radius is 60Δ x =15cm, other areas are vacuum state. The time-harmonic plane wave source is selected as the excitation source, and the expression is E in =sin(2 πf 0 N Δ t ), f 0 Indicates the frequency of the source, and the iteration steps of the electromagnetic simulation are N =1200. Thus running the program, the result is as follows Figure 4 shown. It can be seen in the figure that the truncation boundary is a circle. Figure 4 (a) and (b) are electric fields respectively E z The phase and magnitude of , the inner square is the connecting boundary of the total field and the scattered field in the finite-difference time-domain method. Figure 4 (c) and (d) give ...
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