Originally posted by alexoest
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Sorry to dig up this old thread, but I would like to build pickups of this type myself and I've been thinking about a couple of questions:
It is very good that others are thinking about this!
Would it be possible to just have the primary loop under the strings and connect it by wires to a transformer tucked away in the guitar's control cavity? That'd give a cleaner look.
The short answer is yes but practicaly for only the bridge pickup that is physically closer to the control cavity. So the key question is how do you want to balance the tone of the pickup from the size of the primary loop. Put into scientific language, that means: what is the resistance of the primary loop? You need a primary loop less than about 1 milliohms or 1 one thousandths of an ohm. What is the distance that a continious loop must take to go around the pickup magnetic field (under the strings) and the loop moving inside to the closest place that the current transformer connection can be made? The answer is in your ears! Lower resistance primary loops favors lower frequencies.
Is there a particular reason that you're using a microphone adapter?
Yes!!! The output of the CSE 187L just about matches the input impedance of a Shute A95U matching transformer. But two CSE187L current transformers (CT) allow the outputs to be connected in either series, parallel or single CT, resulting to tonal changes. Where there are changes to be heard is totally dependent on the frequencies we are boosting or cutting compared to the organic sound of a high impedance pickup with 6 to 12 thousand turns of very fine wire. The low impedance pickup has a totaly different and wider bandwidth sound that may not please everyone. However, it has potential upper sound harmonics that can be amplified, if desired.
Couldn't you instead have used any 100:1 current sensing transformer in series with the CSE187L?
The low resistance of the primaty loop allows a vibrating string to produce anywhere between 1 and 10 milliamps at the plucked frequency. String mass, velocity and vibrating frequency all affect the output level. Changing the load on the CT will affect the tonal balance and the amount of gain needed to be recovered in the matching transformer method or in an active amplifier method.
Here, I assume that sending the signal through a 100:1 transformer raises the impedance a hundred times. Is this correct?
No! It changes by the square of the turns ratio. So the CSE187L with a 1 to 500 turns ratio, changes the impedance by 1 to 250,000. Assume that the output load of the CT is 2.500 ohms (like on the Les Paul Low Impedance pickup schematic). Then, the reflected load is 2500 divided by 250,000 or .01 ohms. But you want the source to impedance to be 10 times lower than the load impedance so that means getting a loop resistance in the neighborhood of 1 milliohm or .001 ohms.
And if not, can anyone tell me the correct way to calculate the change in impedance when sending the signal through a transformer?
Last question (for now): What if you instead of just one had about ten primary loops and then send the signal through the 500:1 transformer... would that be equivalent to the around 5000 windings of a traditional pickup?
It is all about how much current is sent through the primary loop. Lower resistance means thicker wire and shorter distances to obtain the right tone to satisfy the ear.
Please enlighten me. I am about to receive a couple of AS104 transformers this week and would like to know some more about the possibilities they give me.
See the posts and posed photos by bajaman on this forum.
/Alex
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