Download this article of VSWR Explained
Here is a useful "cheat sheet" converting VSWR to the percentage of reflected power.
This online VSWR Calculator is also very useful
The lineman sent to locate and correct the fault somewhere along the miles of suspended wirescould at least identify the type of fault by examining the standing wave on the line created by thefault.
This all seems rather primitive, but we should bear in mind that voltage measuring instruments of the day were a delicatemechanism housed in hand-made wooden cases. This made them expensive and fragile, whereas the light bulb was comparatively cheap and robust. The method was cleverer than youmight at first suppose, since it was a form of bolometer able to indicate the RMS value of the two voltage extremes on the line.
Commonplace but pretty much gone in the RF industry by the 1990s, a bolometer fed with RFwould be warmed by the RF resulting in a change in resistance in one arm of a bridge. Theoutput of the bridge gave the RMS value of the RF waveform, no matter how complex thewaveform.
At microwave frequencies slotted lines became a way of accurately determining the ratio of themaximum voltage to the minimum voltage (the VSWR, symbol 's'), and because of the simplicityof measurement and the easy math associated with it, VSWR became an everyday parameter.As the name suggests, a slotted line is a length of waveguide with a slot along the top. A probeis moved along the slot and a detector gives the voltage at any point on the line. Once you haveobtained the two extremes of voltage you can determine the ratio of the two. Once you have thisratio it is easy to calculate the reflected power coefficient, symbol rho. The reflected powercoefficient is the amount of power reflected back compared to the incident power. The AHwebsite has a calculator allowing conversion between s and rho.
Figure 2 is in fact a plot of the detected voltage as the probeis moved along the line This can be misleading since thestanding wave actually goes positive and negative.
Short-Circuit Termination
A voltage cannot exist across a perfect short-circuit, that is the voltage can only have the value0 volts at the short-circuit. A basic law of physics is the conservation of energy. Energy cannotjust disappear, it has to accounted for somehow. Mother Nature gets around the zero voltsrequirement by creating an equal and opposite signal that travels back down the line. At theshort-circuit the +E and -E cancel each other to give the required zero volts.
Open-Circuit Termination
This is the 'dual' of the short-circuit situation. A current cannot flow in a perfect open-circuit, thatis the current can only be zero amps at the open-circuit. Again, Mother Nature gets around thezero amps requirement by creating an equal and opposite signal that travels back down the line.At the open-circuit the +I and -I cancel to give the required zero amps. Technically this shouldbe +H field and -H field, but for our purposes we will stick with +I and -I.
Creation of the Standing Wave
Figures 3(a) and 3(b) show a forward wave and a reflected wave about to 'meet' and interacton a transmission line. The box is our viewing window of the interaction as it occurs. The box isa half-wavelength wide.
Figures 4(a) to 4(m) show the standing wave as the forward and reflected waveforms overlapand add algebraically. The addition is the green trace. Close observation of the green trace inthe observation window shows it stands still, that is it pulses positive and negative, but stays inthe same place along the line. Hence the name Standing Wave
At last the acronym Voltage Standing Wave Ratio makes sense.
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