W9TR
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A conductor moving in a magnetic field will create a voltage proportional to the length of the conductor, the strength of the magnetic field, and the velocity the conductor is moving through the magnetic field.
emf=l*h*v
This is Faraday’s Law.
l=length of the conductor in meters
h=field strength in Tesla’s
v=velocity of the conductor in meters/sec.
The earth’s magnetic field is about 0.00005 Tesla.
A 1m cable vibrating with a velocity of 1 m/s would create. 50 uV signal which is actually well above the noise floor of a good system.
Here is the derivation.
I used a sine wave in the analysis to make the math simple. Arbitrary waveforms can be analyzed using Fourier analysis.
The amplitude A of a vibration needed to create a velocity v of the same conductor is simply A=v/w where w= angular velocity = 2*Pi*f where f = frequency of the vibration.
So, at 1 kHz and a velocity of 1 m/sec we get an amplitude of 160 microns. About the width of a human hair. Slightly larger than an RCH, probably about the same width as a muggeseggele. (Look it up)
Is this audible? I don’t know and it’s not my purpose here to make that call. Believers will believe, non-believers won’t - pretty cut and dried.
Suffice it to say that a small amount of movement in a wire is enough to create a voltage that will turn your beautiful 24 bit signal (really only 21 bits but that’s a subject for another day) into a 14 bit one.
Somebody asked about vibration effects on other electronic components. Sure, there are plenty. Common ceramic capacitors with high Q dielectrics like X7R and COG exhibit piezoelectric properties and so can create voltages under vibration. This is especially true of MLCC SMT capacitors. Other large film and foil capacitors will also exhibit value modulation under vibration. The Crystal oscillators that are so foundational to digital audio are very susceptible to even small vibrations, which modulate their output frequency.
emf=l*h*v
This is Faraday’s Law.
l=length of the conductor in meters
h=field strength in Tesla’s
v=velocity of the conductor in meters/sec.
The earth’s magnetic field is about 0.00005 Tesla.
A 1m cable vibrating with a velocity of 1 m/s would create. 50 uV signal which is actually well above the noise floor of a good system.
Here is the derivation.
I used a sine wave in the analysis to make the math simple. Arbitrary waveforms can be analyzed using Fourier analysis.
The amplitude A of a vibration needed to create a velocity v of the same conductor is simply A=v/w where w= angular velocity = 2*Pi*f where f = frequency of the vibration.
So, at 1 kHz and a velocity of 1 m/sec we get an amplitude of 160 microns. About the width of a human hair. Slightly larger than an RCH, probably about the same width as a muggeseggele. (Look it up)
Is this audible? I don’t know and it’s not my purpose here to make that call. Believers will believe, non-believers won’t - pretty cut and dried.
Suffice it to say that a small amount of movement in a wire is enough to create a voltage that will turn your beautiful 24 bit signal (really only 21 bits but that’s a subject for another day) into a 14 bit one.
Somebody asked about vibration effects on other electronic components. Sure, there are plenty. Common ceramic capacitors with high Q dielectrics like X7R and COG exhibit piezoelectric properties and so can create voltages under vibration. This is especially true of MLCC SMT capacitors. Other large film and foil capacitors will also exhibit value modulation under vibration. The Crystal oscillators that are so foundational to digital audio are very susceptible to even small vibrations, which modulate their output frequency.