If anyone wants to do some quick and inexpensive current sensing experiments do a web search for the following low frequency current sensing transformer: CSE187L. It costs about $2.50 and less in quanties. It has a 1:500 turns ratio with the primary having a "U" shaped single turn through the core using very heavy wire with a 250 micro ohm resistance (AWG 12 about 2 inches long). The secondary has 21 ohms of resistance.
My quick experiments were done using a Tenma 72-6950 audio impedance meter which has a range of 1 to 2000 ohms in three ranges, X1, X10, X100.
The secondary impedance of the CSE187L has close to 500 ohm impedance when the low impedance input is properly loaded down. The reflected impedance is very sensitive to the primary loading and is reflected by the high turns ratio. Using 12 turns of AWG 18 on the 3/16" rod magnet resulted in about 1200 ohm reflected impedance.
I used 4 turns of AWG 18 around a 3/16" magnet and directly connected it to the transformer right next to the coil and got about 50mv output. The peak was closer to 100mv. When I connected it to a 500 ohm to 50K ohm Shure matching transformer, I got an output in the range of a typical guitar pickup. This adds another 1:10 output voltage boost. So, now with both transformers there is a 1:5000 voltage boost, less the losses in the transformers. This means that the output efficiency is very closly related to the current induced in the primary, the size of the wire and number of turns.
Here is where you could get some house hold copper wire, AWG 12 to 14 and strip off a six inch length, make one U-shaped loop around a magnet and get some measurable output on a scope and listening through a guitar/bass amp. You can add more turns to try to optimize the output but here the thickness of the wire and the connection to the transformer primary is critical. Look for some thin copper tubing the same ID as the transformer primary wire to make a quick coupling mechanism. This will allow you making quick changes while experimenting.
Measuring the impedance of four turns of AWG 18 reflects an output impeance on the transformer of about 600 ohms and increases by only 100 ohms when the manget slug in inserted in the center of the coil. This should give the experimenters some idea about how sensitive the low-Z side is to generating enough current to optimize the primary connection.
The specification sheet suggests a 60 ohm load resistor on the transformer secondary. I suspect that the optimum loading would occur when the primary reflects a 60 ohm secondary impedance. This would imply that the optimum impedance/resistance of the primary should be no more than 0.0154919 ohms (square root of 60 divided by 500) However, to obtain the maximum voltage output, a 10 X impedance loading of 600 ohms might be better. Anyone have any ideas on this?
Look at Lace Alimnitone pickups and see how thick the primary winding are. These are the actual aluminum loops around the magnet. The transformer is underneath coupled directly to the aluminum loops.
To minimize noise, run a short jumper from one side of the primary to the ground side of the secondary. I'm sure that someone could figure out how to make this a balanced output with the signal leads floating to feed a balanced input to the matching transformer like the Shure A95U pluged in directly to the amp input.
This current sensing pickup winding method would make a new breed of pickups that could be made very easy, have a wide bandwidth response, have minimal susceptibility to external noise, allow longer cable runs, and use a commonly available externally connected 500 ohm to 50K ohm matching transformer.
If anyone try this experiment, keep good notes about the wire size, number of turns around the magnet, transformer type, and total length of the primary winding around the magnets so you can post the results here so we can all benefit from the collective efforts of the pickup builder community.
Hopefully this post will get the ball rolling.
Joseph J. Rogowski
My quick experiments were done using a Tenma 72-6950 audio impedance meter which has a range of 1 to 2000 ohms in three ranges, X1, X10, X100.
The secondary impedance of the CSE187L has close to 500 ohm impedance when the low impedance input is properly loaded down. The reflected impedance is very sensitive to the primary loading and is reflected by the high turns ratio. Using 12 turns of AWG 18 on the 3/16" rod magnet resulted in about 1200 ohm reflected impedance.
I used 4 turns of AWG 18 around a 3/16" magnet and directly connected it to the transformer right next to the coil and got about 50mv output. The peak was closer to 100mv. When I connected it to a 500 ohm to 50K ohm Shure matching transformer, I got an output in the range of a typical guitar pickup. This adds another 1:10 output voltage boost. So, now with both transformers there is a 1:5000 voltage boost, less the losses in the transformers. This means that the output efficiency is very closly related to the current induced in the primary, the size of the wire and number of turns.
Here is where you could get some house hold copper wire, AWG 12 to 14 and strip off a six inch length, make one U-shaped loop around a magnet and get some measurable output on a scope and listening through a guitar/bass amp. You can add more turns to try to optimize the output but here the thickness of the wire and the connection to the transformer primary is critical. Look for some thin copper tubing the same ID as the transformer primary wire to make a quick coupling mechanism. This will allow you making quick changes while experimenting.
Measuring the impedance of four turns of AWG 18 reflects an output impeance on the transformer of about 600 ohms and increases by only 100 ohms when the manget slug in inserted in the center of the coil. This should give the experimenters some idea about how sensitive the low-Z side is to generating enough current to optimize the primary connection.
The specification sheet suggests a 60 ohm load resistor on the transformer secondary. I suspect that the optimum loading would occur when the primary reflects a 60 ohm secondary impedance. This would imply that the optimum impedance/resistance of the primary should be no more than 0.0154919 ohms (square root of 60 divided by 500) However, to obtain the maximum voltage output, a 10 X impedance loading of 600 ohms might be better. Anyone have any ideas on this?
Look at Lace Alimnitone pickups and see how thick the primary winding are. These are the actual aluminum loops around the magnet. The transformer is underneath coupled directly to the aluminum loops.
To minimize noise, run a short jumper from one side of the primary to the ground side of the secondary. I'm sure that someone could figure out how to make this a balanced output with the signal leads floating to feed a balanced input to the matching transformer like the Shure A95U pluged in directly to the amp input.
This current sensing pickup winding method would make a new breed of pickups that could be made very easy, have a wide bandwidth response, have minimal susceptibility to external noise, allow longer cable runs, and use a commonly available externally connected 500 ohm to 50K ohm matching transformer.
If anyone try this experiment, keep good notes about the wire size, number of turns around the magnet, transformer type, and total length of the primary winding around the magnets so you can post the results here so we can all benefit from the collective efforts of the pickup builder community.
Hopefully this post will get the ball rolling.
Joseph J. Rogowski
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