For a lossless line with a characteristic impedance that is real, terminated in a resistive load.
Avoiding common scale factors.
The incident wave at the load will be Ei = Sin(t).
At a point a time x before the load, Ei = Sin(t+x).
The reflected wave will have an amplitude, A, between –1 and +1, determined by Zo and R.
The reflected wave at the load will be Er = A*Sin(t).
At a point back up the line, a time x after reflection from the load, Er = A*Sin(t–x).
Then the sum of the incident and reflected waves is Es = Ei + Er = Sin(t+x) + A*Sin(t–x)
For values of x = wave period * n / 4 ; there will be maxima and minima in Es.
Es = Sin(t+x) + A*Sin(t–x) represents the standing wave.
legyptien21 said:
Vr*(sin (wt - kx) + sin (wt + kx)) represent a standing wave if we use the Simpson formula...
That should be Es = Vi * Sin(wt + kx) + Vr * Sin(wt - kx)