With regard to the original question; any complex circuit can be simplified for the purpose of analysis. How the simplified model then holds up in real life is another matter.
Whilst adding capacitance to one end to make up the measurable capacitance gives the same reading, in reality your cable has distributed capacitance. This means that there are an infinite number of parallel capacitors, and an infinite number of series resistances, as well as an infinite number of inductors. When you measure a cable at the end you're seeing the total of all of these.
Distributed capacitance acts differently than just adding a capacitor at one end, but is probably not detectable to the ear at audio frequencies. At RF it shows up in how intermodulation frequencies get attenuated along a transmission line.
Whilst adding capacitance to one end to make up the measurable capacitance gives the same reading, in reality your cable has distributed capacitance. This means that there are an infinite number of parallel capacitors, and an infinite number of series resistances, as well as an infinite number of inductors. When you measure a cable at the end you're seeing the total of all of these.
Distributed capacitance acts differently than just adding a capacitor at one end, but is probably not detectable to the ear at audio frequencies. At RF it shows up in how intermodulation frequencies get attenuated along a transmission line.
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