Transparent excitation source implementation method applied to finite-difference time-domain method
A technology of finite difference in time domain and implementation method, which is applied in the field of computational electromagnetics and can solve problems such as reducing computational efficiency
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[0130] The present invention will be described in further detail below in conjunction with the accompanying drawings and embodiments.
[0131] In the example, the model of two two-dimensional uniform waveguides scattering at the junction is tested, such as Figure 5 shown. The width of the first waveguide is a=22.86mm, the width of the second waveguide is a / 2, the simulation parameters are: space step Δx=Δz=1.143mm, Δt=0.0019ns, simulation time step nt=900. Incentives employ a TE 10 A cosine-modulated Gaussian pulse of the mode, center frequency f 0 =16GHz, the excitation source is loaded on the input port of the first waveguide, and the equation of the excitation source added is
[0132]
[0133] Among them, n 0 =450,n d =125.
[0134] step 1,
[0135] All electromagnetic field components distributed at the excitation source grid have three sets of values, E Py 、H Pz ,E Ny 、H Nz and E Ry 、H Rz .
[0136] Step 2. According to the excitation source equation f ...
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