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codes (2)
Electromagnetic wave propagation tool
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Application background This is a set of tools in Python language for easily simulating parameters related to propagation of uniform plane waves (UPW) such as its phasor (in case of time harmonic plane waves), group velocity, oblique incidence, reflection and the standing wave pattern created by reflection. The tool set also simulates parameters related to different antenna's arrangements like linear antenna and array of antennas. Key Technology These codes are related to the intermediate knowledge of electromagnetic theory. Once you understand Maxwell equations the next step is understanding the concept of electromagnetic waves propagation and its simplest and most important case (uniform plane waves). This theory is basically the same of transmission lines and is the base to guided waves, antenna and microwaves engineering theories. These theories are essential to almost all modern consumer electronic devices and countless other RF dev
abel12345
2016-08-23
0
1
Plane wave of uniforma oblique incidence
no vote
Application background This code simulates a few parameters related to oblique incidence of uniform plane waves, just angle of refraction, intrinsic impedance on second mean, amplitude of the magnetic field etc This code also works when the angle of incidence is bigger than the critic angle. In such situation, the intrinsic impedance becomes complex, there's no propagation of energy to the second mean and a evanescent wave appears. (You can see this through the H amplitude etc) Key Technology This code is related to the intermediate knowledge related to electromagnetic theory. Once you understand Maxwell equations, the next step is understanding the concept of electromagnetic waves and its simplest and most important case (uniform plane waves). This theory is basically the same of transmission lines and is the base to guided waves, antenna and microwaves engineering theories. These theories are essential to almost all modern consumer and RFI
abel12345
2016-08-23
1
1
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