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The multipath component is parameterized by calculating the reflected fields from the floor, ceiling and walls of the indoor environment as well as scattered fields from moving human bodies which are modeled as finite dielectric cylinders.
The multipath component is parameterized by calculating the reflected fields from the floor, ceiling and walls of the indoor environment as well as scattered fields from moving human bodies.
Moreover, the equivalent circuit and transmission line model are derived based on the reflected fields and vector-fitting method to facilitate analysis of the proposed design and evaluation of the full-wave simulation results.
These two reflected fields give rise to an observable interference signal.
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If we assume for the moment that the JPA has no internal losses, all the incident power is reflected from the resonator and the classical response (i.e. reflection coefficient) is completely specified by the phase φ of the reflected field.
The direct wavenumber spectrum is then combined with the plane wave reflection coefficient of the impedance plane to yield the wavenumber spectrum of the reflected field.
We depict the reflected field amplitude graphically for various dimensions of the given waveguide.
The following relation can be derived for the reflected field amplitude.
The multi-level, fast multipole method (MLFMM) is used to accelerate internal reflected field calculation.
We also depict some graphical representations by determining the reflected field amplitude for various dimensions of the pentafurcated duct.
Similarly, we present the graph of the reflected field amplitude versus the wave number k in Figure 6.
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