A guitar or bass with metal strings has the potential to utilize a new way to sense the vibrations from the string. Just think of a metal string as a "moving conductor" or a "wire in a magnetic field" (web search on the words within quotes for more information).
I'll share with you what I have learned from tinkering with pickups for almost 50 years.
A voltage can be generated when a wire is moved through a magnetic field. To see this with a quick experiment do this. Use an acoustic guitar and attach a scope probe across one string then move a cermic magnet near the string. Set the scope the a low mv range. Plunk the string and you will see an output in the 2 to 5 mv range. Just like traditional high impedance pickups with thousands of coil turns around magnets, the output of the string motion is a function of the actual motion vector at right angles to the field direction. This is defined a Lorentz Voltage.
Lorentz Voltage is defined as E=LB dx/dt sin (/) (my poor excuse for a Greek letter) where:
dx/dt is the velocity of the moving conductor;
B is the strength of the magnetic field;
L is the length of the conductor in the magnetic field; and
(/) is the angle of the direction of conductor motion relative to the direction of the magnetic field.
Based on the above formula and my own experiments, the voltage induced within the string increases as the length of the magnetic field is increased. I used a .5" wide by 6.5 " long by 0.125" thick rubberized magnet running under the string from the end of the fingerboard to near the bridge. By adjusting the magnet height to be closer to the string near the bridge I can balance the harmonic output. This arrangement puts a full quarter string length within the magnetic field.
Now for the fun part. Obtain a low frequency current transformer such as a "CSE187L" for about $2.50 (single unit price) from Allied or Jameco. If you have a scope current probe you can use this also by just putting the probe around the string behind the nut and use a thick jumper wire to connect the string behind the probe and the bridge end of the same string. This now forms a single turn loop with the string acting as the ribbon in a "ribbon microphone". Use the CSE187L by attaching the primary (single turn transformer wire) to the string with jumper wires attached to the string behind the nut and behind the bridge. Attach your scope or amp to the secondary and observe or listen to the sound. The output of the CSE187L is about 21 ohms DCR and matches a low impedance XLR to high Z matching transformer 500 to 50,000 ohms at a 1:10 turns ratio very well or a microphone mixer XLR input.
The CSE187L has a 1:500 turns ratio and is rated for a 50 to 400Hz frequency range but it goes well beyond that. You can even connect two strings in series by electrically connecting the individual machine heads of the bass E and A strings together and attach the CSE187L primary behind the bridge to these two strings and make a quick two string pickup for test purposes.
For a little more output you can obtain a "low frequency torroid current transformer" with turns ratios up to 1: 3000. Just run a jumper from the string behind the nut, loop it through the torroid as the primary loop and connect the other end behind the bridge.
You might ask, why has this pickup not been popular?
1. You need to have a ground return from the strings at the nut end into the body of the guitar near the bridge.
2. It does not just drop in with a standard single coil or humbucker footprint.
3. The strings can act as an antenna and pickup hum.
As another experiment take a soldering gun and use it as a hum source. When a single string or two series strings are connected to an amplifier, move the soldering gun near the string and listen to the hum.
Here is the challenge for the technically curious.
(1) How could you apply traditional humbucking techniques from traditional high impedance pickups to this moving coil pickup?
(2) Using the current transformer techniques described above, how could you adjust the output level of each string to obtain a more acoustically balanced string output.
(3) What other musical applications can be derived form having individual and isolated string outputs.
I hope this stimulates some thinking and introduces another approach to making guitar pickups. I hope some of you try these quick experiments and share your results.
Joseph Rogowski
I'll share with you what I have learned from tinkering with pickups for almost 50 years.
A voltage can be generated when a wire is moved through a magnetic field. To see this with a quick experiment do this. Use an acoustic guitar and attach a scope probe across one string then move a cermic magnet near the string. Set the scope the a low mv range. Plunk the string and you will see an output in the 2 to 5 mv range. Just like traditional high impedance pickups with thousands of coil turns around magnets, the output of the string motion is a function of the actual motion vector at right angles to the field direction. This is defined a Lorentz Voltage.
Lorentz Voltage is defined as E=LB dx/dt sin (/) (my poor excuse for a Greek letter) where:
dx/dt is the velocity of the moving conductor;
B is the strength of the magnetic field;
L is the length of the conductor in the magnetic field; and
(/) is the angle of the direction of conductor motion relative to the direction of the magnetic field.
Based on the above formula and my own experiments, the voltage induced within the string increases as the length of the magnetic field is increased. I used a .5" wide by 6.5 " long by 0.125" thick rubberized magnet running under the string from the end of the fingerboard to near the bridge. By adjusting the magnet height to be closer to the string near the bridge I can balance the harmonic output. This arrangement puts a full quarter string length within the magnetic field.
Now for the fun part. Obtain a low frequency current transformer such as a "CSE187L" for about $2.50 (single unit price) from Allied or Jameco. If you have a scope current probe you can use this also by just putting the probe around the string behind the nut and use a thick jumper wire to connect the string behind the probe and the bridge end of the same string. This now forms a single turn loop with the string acting as the ribbon in a "ribbon microphone". Use the CSE187L by attaching the primary (single turn transformer wire) to the string with jumper wires attached to the string behind the nut and behind the bridge. Attach your scope or amp to the secondary and observe or listen to the sound. The output of the CSE187L is about 21 ohms DCR and matches a low impedance XLR to high Z matching transformer 500 to 50,000 ohms at a 1:10 turns ratio very well or a microphone mixer XLR input.
The CSE187L has a 1:500 turns ratio and is rated for a 50 to 400Hz frequency range but it goes well beyond that. You can even connect two strings in series by electrically connecting the individual machine heads of the bass E and A strings together and attach the CSE187L primary behind the bridge to these two strings and make a quick two string pickup for test purposes.
For a little more output you can obtain a "low frequency torroid current transformer" with turns ratios up to 1: 3000. Just run a jumper from the string behind the nut, loop it through the torroid as the primary loop and connect the other end behind the bridge.
You might ask, why has this pickup not been popular?
1. You need to have a ground return from the strings at the nut end into the body of the guitar near the bridge.
2. It does not just drop in with a standard single coil or humbucker footprint.
3. The strings can act as an antenna and pickup hum.
As another experiment take a soldering gun and use it as a hum source. When a single string or two series strings are connected to an amplifier, move the soldering gun near the string and listen to the hum.
Here is the challenge for the technically curious.
(1) How could you apply traditional humbucking techniques from traditional high impedance pickups to this moving coil pickup?
(2) Using the current transformer techniques described above, how could you adjust the output level of each string to obtain a more acoustically balanced string output.
(3) What other musical applications can be derived form having individual and isolated string outputs.
I hope this stimulates some thinking and introduces another approach to making guitar pickups. I hope some of you try these quick experiments and share your results.
Joseph Rogowski
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