most of the people talking about impedance and capacitance seem to think we all work in the RF spectrum. we don't. we are in the VERY low frequency spectrum. the effects are minimal, as to be ignorable.
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I'll second the GeorgeL's recommendation, I've tried most of the "high end" cables out there and find the GeorgeL's (.225) to be some of the clearest sounding cables for sure.
Capacitance of the cables is not insignificant, even for bass. The problem is that the output impedance of passive instruments and the input impedance of instrument amps are REALLY HIGH so that even a small capacitance makes a high-frequency roll-off filter, well into the audio frequencies. This type of filter also causes a phase delay, "smearing" your transients and attacks. The longer the cable, the worse the roll-off.
If you want all the sound you are making, ,the ELIXIR cables have the lowest capacitance per foot of any cable out there and will provide the cleanest sound. It is clearly audible unless you play in the mud.
but what it is also basicaly doing is making your bass hot... which would make you ground.
most of the people talking about impedance and capacitance seem to think we all work in the RF spectrum. we don't. we are in the VERY low frequency spectrum. the effects are minimal, as to be ignorable.
No, just the shield is connected to only one side, but there is still a common ground wire running the whole length. Often these types of cables use a twisted pair for the signal conductors.
The idea is to keep the shield separate from the signal ground.
To think that because you play a bass guitar that the only frequency content of your signal is in the sub-2500Hz range is ignorant. There is harmonic information in your signal all the way out past 20kHz although it is at a lower level than the fundamental. It the very same reason that vinyl LPs sound vastly different than a 320kpbs MP3 file.
A cable is a very complex passive signal filter. It has capacitance, inductance and resistance, not to mention than different dielectrics will absorb re-release energy randomly into the signal at different rates.
most of the people talking about impedance and capacitance seem to think we all work in the RF spectrum. we don't. we are in the VERY low frequency spectrum. the effects are minimal, as to be ignorable.
are you sure?
on instrument cable there is usaly only 2 conductors... the shield and the center.
for that to work you would need a stereo jack, something I have never seen on an instrument cable, or an amplifier.
yes I know, but even up past 20khz these things have very little effect.
That's not true at all. Why do you think it is?
now that was just quick so I am sorry if it is not very accurate... but I don't know many Cabs that can even reproduce a sound down to 45 hZ and the ear can only hear usuay down to 32 Hz...
I stand by my opinion.
You don't hear the fundamental on your low E string (or your low B)... it's too low, but you do hear the harmonics. And the cable is affecting the harmonics.
You can hear the fundamental if you remove the harmonics. Try it with a signal generator and see.
A cable is a very complex passive signal filter. It has capacitance, inductance and resistance, not to mention than different dielectrics will absorb re-release energy randomly into the signal at different rates.
because I am an RF engineer and these things are MAJOR to us.
at lower frequencies the effect are negligable.
When signals flow in cables, some energy is stored in the electric and magnetic fields within and surrounding the cable. This energy propagates along the length of the cable, forming a transmission line. Such effects as reflections, standing waves or frequency response ripples will occur unless this energy is absorbed at each physical end of the cable. Depending on its construction, every cable has a characteristic impedance, which is the impedance required to perfectly absorb the energy or terminate each end.
Cable capacitance is the dominant problem for audio lines more than approximately 100 feet (30 m) long. As shown in Figure 1, a low-pass filter is formed by the driver's output impedance and the capacitance of the cable. The bandwidth of this filter becomes lower as output impedance and cable length increase. It is especially important to consider that typical unbalanced (RCA jack) consumer equipment can have a 1 kV or higher output impedance (not usually specified either). The bandwidth is f = 1 (2p infinity R infinity C), where f is the -3 dB frequency in Hz, R is the driver output impedance in ohms, and C is the cable capacitance in farads. For example, consider an unbalanced consumer output, where R = 1 kV, which drives 200 feet of 50 pF/ft cable where C = 10 nF. In this example, response will be down 3 dB at 16 kHz. Another example would be a balanced pro output, where R = 200 V, which drives 3,000 feet of 18 pF/ft shielded twisted-pair cable where C = 54 nF. In this exam! ple, response will be down 3 dB at 14 kHz.
Another, less recognized, problem associated with cable capacitance is limited driver output current.
Ground noise and interference
Simply because of the physical distances involved, significant ground voltage differences between driver and receiver are almost certain with long lines. Ground voltage differences, because they are generated by normal power line leakage currents, are heard as a noisy mix of hum, buzz, pops, clicks and other rude noises, which I collectively call "ground noise." Unbalanced lines are susceptible to enormous problems in this regard because the ground noise across the length of the shield couples directly into the received signal
not gonna get into an argument with you about this but I don't agree with you.
here is a good article on resonance and how cables work.
http://www.audioholics.com/education/cables/debunking-the-myth-of-speaker-cable-resonance
when using this calculator
Invalid Link Removed
for a 20 foot cable I get around 0.2 nF
so lets make a rc filter out of that.
the cutoff frequency of a rc filter is
Fc=1/2piRC
so after some quick research and amp input is usualy 3.9 Mohms...
so the formula is
FC= 1/2(3.14)(3.9x10^6)(0.2x10^-9)
FC= 1/2(3.14)(0.00351)
FC= 1/2(0.0110214)
FC= 1/0.0220428
FC= 45.36 Hz
now that was just quick so I am sorry if it is not very accurate... but I don't know many Cabs that can even reproduce a sound down to 45 hZ and the ear can only hear usuay down to 32 Hz...
I stand by my opinion.