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The lineman sent to locate and correct the fault somewhere along the miles of suspended wires could at least identify the type of fault by examining the standing wave on the line created by the fault.
The lineman would gauge how brightly a light bulb connected across the line would glow as the connection was moved along the line (Figure 1(b)). If the bulb lit brightly at one place on the line and would not light at all further along the line, then he knew to look along the line for an open or short circuit. If the bulb was fairly bright at one place and somewhat dimmer in another, he knew to look for a partial short across the wires.
This all seems rather primitive, but we should bear in mind that voltage measuring instruments of the day were a delicate mechanism 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 you might 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 RF would be warmed by the RF resulting in a change in resistance in one arm of a bridge. The output of the bridge gave the RMS value of the RF waveform, no matter how complex the waveform.
At microwave frequencies slotted lines became a way of accurately determining the ratio of the maximum voltage to the minimum voltage (the VSWR, symbol 's'), and because of the simplicity of 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 probe is moved along the slot and a detector gives the voltage at any point on the line. Once you have obtained the two extremes of voltage you can determine the ratio of the two. Once you have this ratio it is easy to calculate the reflected power coefficient, symbol rho. The reflected power coefficient is the amount of power reflected back compared to the incident power. The AH website has a calculator allowing conversion between s and rho.
Note, many textbooks portray a standing wave as shown in Figure 2.
Figure 2 is in fact a plot of the detected voltage as the probe is moved along the line This can be misleading since the standing wave actually goes positive and negative.
A voltage cannot exist across a perfect short-circuit, that is the voltage can only have the value 0 volts at the short-circuit. A basic law of physics is the conservation of energy. Energy cannot just disappear, it has to accounted for somehow. Mother Nature gets around the zero volts requirement by creating an equal and opposite signal that travels back down the line. At the short-circuit the +E and -E cancel each other to give the required zero volts.
This is the 'dual' of the short-circuit situation. A current cannot flow in a perfect open-circuit, that is the current can only be zero amps at the open-circuit. Again, Mother Nature gets around the zero 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 should be +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 interact on a transmission line. The box is our viewing window of the interaction as it occurs. The box is a half-wavelength wide.
Figures 4(a) to 4(m) show the standing wave as the forward and reflected waveforms overlap and add algebraically. The addition is the green trace. Close observation of the green trace in the observation window shows it stands still, that is it pulses positive and negative, but stays in the same place along the line. Hence the name Standing Wave
At last the acronym Voltage Standing Wave Ratio makes sense.
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