These three videos show the behavior of a standing wave. In this first one we can see a perfect standing wave. This wave is produced as a sum of two waves of the same amplitude, flowing in the same direction but in opposite sense. You can observe that there are positions where the wave amplitude is always zero and also, that there are instants that the amplitude is zero everywhere.
A voltage standing wave can be generated when a transmission line ended in a pure imaginary load, as for example a short circuit:
It is easy to realize that it is a short circuit, because the voltage is equal to zero at the end.
What happens if these waves have different amplitude? This is the general case, when a transmission line is ended in an arbitrary load:
We can see that a wave is flowing towards the positive sense. Also, a backward wave with lower amplitude is flowing in the line. The sum of both waves produce a net flux of energy toward the positive sense and also standing wave.
This simulation shows the behavior of a lossy transmission line (TL). A sinusoidal signal propagates through the TL and, due to the losses, the signal decays when it advances. If you stop the motion at t=8s and join the peaks with an imaginary line, a decreasing exponential can be sketched. Moreover, this TL is not matched. It is very difficult to see the backward wave because it has very low level. However, if you stop the motion at t=10 s, you can see that the waveform at the end of the line is different to the waveform at the beginning.
This video represents the potential and the intensity of two different Transmission Lines (TLs) joined in cascade. This simulation is made using the Finite Different Time Domain (FDTD) method, which allows us to visualize what happens when the time goes by.
What can we see? A step signal feeds the first TL and the line is excited by certain potential. At t=2s, the step arrives to the discontinuity between the two TLs. Two waves appear: one wave is generated in the second line to forward direction and another wave advances to the backward direction. The first TL has a bigger transmission speed than the second. The wave in the second line arrives at t=8s to a certain load and a backward wave is produced that come back to the discontinuity.
Let‘s look a little more inside. We can make some affirmations. Try to understand why:
– The two lines are lossless.
– The two lines have different transmission speed and different impedance. The impedance of the first line is smaller than the second one.
– The load at the end of the second TL has a real value smaller than the impedance of the second line
– The generator is matched to the first TL.
This is a very interesting project in which my group is involved.
You can have more information in Catedra Telefónica – Universidad de Oviedo
This is a great work of the Microwave Group of the Universidad de Sevilla, where I began my research.
This is the research group I was visiting in October 2013.
I was not working on meta-materials. I was measuring some mm-wave lens. It was a great time.