Most of those "brass" jumpers are probably brass or cadmium plated steel.
And since iron and steel have six times the resistivity of copper, not to mention the phase changes caused by the different reactances... From there on it gets really testical...
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These cable type threads always end up talking b####x! Got my granny to knit some speaker jumpers. Maybe she used too heavy a gauge as the sound became all woolly. Removed them again and it was like a veil had lifted.
FWIW I just pass the cable through the low connector, de-nuding enough cable for it to clamp down and terminate it on the high connector. Something about using one continuous piece of wire makes sense to me. It doesn't really sound a world different to other configurations.
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Aristotle is supposed to have said "The more you know, the more you know you don't know." The flip side of that is that "the less you know, the less you don't know what you don't know". Therefore Just because YOU don't understand something doesn't make it ball-cocks.
My degree is in mechanical engineering, but it included enough electrical engineering, and my experience with 30 years designing and spec-ing subsea power cables in umbilicals, has taught me there's a darned sight more to cable design than simply the cross sectional area, DC-resistivity and length. Stuff like the capacitance of the cables, the dilectric coefficients of the insulators, how the impedance varies not only with current, but also the temperature of the cable, the frequency of the signal, etc. Our cable engineers go to great lengths (cough) to ensure that signals actually make it to the ends of these very long (30+mile) cables, and don't fizzle out half-way along (that's called attenuation by the way).
Let's start with a simple DC circuit, like, say, a bicycle light. A battery operated device where a DC current goes through an incandescent bulb, which, one it gets to a constant temperature, has a static, Ohms Law only resistance. If we neglect the drop in battery output over a short time period, there is no alternating or dymanic element to the voltage, and therefore the current is constant. Therefore the reactive elements of the conductors and the bulb don't come into play.
In a speaker circuit, however, the signal is dynamic. It rises and falls according to the volume, and it's frequency varies according to the notes being played. Therefore the cable's impedance rather than its resistance comes into play and that can and does affect how quickly different frequencies make it along a cable. All conductors have both a resistive (static or DC if you like) element and a reactive (or AC if you like) element that adds up to the total impedance (rather than basic Ohm's Law resistance) of the cable. Impedance is usually expressed as the square root of the sum of the resistive element squared and the reactive element squared (a bit like Pythagorus).
Now, comparing a cable to a brass (or steel or chewing gum for that matter) jumper, it should be bleeing obvious that a collection of, a PAIR of say 39 copper strands, helically would together, then wrapped in a poly-something-or-other insulating layer, then bunched under an outer sheath over that, looks a lot like a lot like a capacitor (two conductors separated by an insulating material), whereas two metal stips in isolation look a lot more like very simple 1-turn or zero-turn coils. In a capacitor the current leads the voltage by 90 degrees (or a quarter cycle if you like). In a coil, the current lags the voltage by the same 90 degrees. So now you've gone from a situation where the current, which was leading the voltage in the cable, now gets forced to lag the voltage in the jumper. This introduces a phase shift and that's why jumpers often make the sound, erm, sound, so naff.