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It can be convenient to define a reference impedance for S-paramters
which is not the characteristic impedance of all the pieces of transmission line in the system, and keep the same reference impedance for all your work. For example, 50 ohms is commonly used, even though the system contains sections of microstrip of various impedances. But that's just a convenience for system analysis and design. If you want to try to assign even a little physical significance to reflection coefficient as used on a piece of line, you really should be using the line's characteristic impedance as the reference impedance. In addition, you should realize that it's going to make sense only in a linear, time-invariant system with steady-state excitation, with only one source of excitation (at a time). In addition, it is of course a function of frequency, just as the line's characteristic impedance is. As others have noted, the magnitude of the reflection coefficient can be greater than unity with a passive line and load. Don't try to read too much physical significance into that, however. Although the classic definition of (V)SWR involves knowing a voltage maximum and a voltage minimum on a line, I much prefer a definition in terms of forward and reverse voltages. That allows me to think about SWR at a point on a uniform line, and realize that it will be different at different points (because of line attenuation). In fact, the _definition_ I use for reflection coefficient is Er/Ef, or equivalently the ratio of electric fields (or magnetic fields) associated with forward and reverse waves (which then applies also to non-TEM waveguides). From that definition, it's straightforward to determine that rho = (Zl-Zo)/(Zl+Zo). And in keeping with the idea that you cannot have a voltage magnitude minimum less than zero, and because I believe it's more practical than the classic definition to have an SWR definition I can apply to any point on a line, my working SWR defintion is SWR = (|Ef|+|Er|)/(|(|Ef|-|Er|)|). This will align well with the usual formula that SWR = (1+|rho|)/(1-|rho|) when |rho|=1, but it never gives you a negative SWR. If you can accept my definition of SWR, we can talk about SWR. If you can't, then I just won't talk with you about SWR, and limit the discussion to reflection coefficient which we presumably would be able to agree on. Cheers, Tom (Dr. Slick) wrote in message . com... From Pozar's Microwave Engineering (Pg. 606): Reflection Coefficient looking into load = (Zl-Zo)/(Zl+Zo) Where Zl is a purely real load impedance, and Zo is the purely real characteristic impedance reference. When you change Zo, you change the normalized center of the Smith Chart, and therefore the Reflection Coefficient and SWR, looking into the same load. Check it out... Slick |
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