ltournell
TDPRI Member
Hello,
Following our previous topic here , this is a more complete and synthesized analysis (or an attempt to ) of the SOLDANO SLO 100-50 and 30 preamp . Remember that the point was to discover the part of that strange 3rd stage in the schematics of the OD channel here below :
The LTSpice simulation was therefore made from this schematic in which the red arrows show where the loaded output of the previous stage was measured :
The various computations made from the load lines and the correct formulas give this table :
Remember the low cut-off frequency due to the cathode RkCk network is given by :
The purpose is to characterize the sounds produced and more particularly the nature of the harmonics of the overtones resulting from overdriving the stages. We can make out the rate of ODD harmonics and EVEN harmonics.
So to start with we simulate with very common guitar PUs : the 490R and 498T Gibson humbuckers for which an approaching value of the ATTACK level can be found in the next table :
For example we see that the 498T outputs the maximum level with the 6th string at 1 Vpp , so the first stage with its 3 Vpp headroom will in no way be overdriven , which is a good thing since this stage is shared with the clean channel !
Now the complete channel is controlled with only one pot and it will be interesting to make it vary on the full range to see where we go : the lower values will be usefull to see what happens in the decreasing tails of the sustained overdriven notes.
Now the "log" pot . Of course with 11 graduations it is more precise than with 10 but for the computations it will be more simple to take 10 . Of course real logarithmic pots only exist in laboratories and not in our amps. What we call log pots are simply 2 linear pots in series , the second one having a far steeper slope than the first one . For each graduation the percentage of the input signal is this one :
So now I suggest we take a breath (
) before we :
1. measure the various outputs of the stages with various inputs
2. identify for the various outputs the harmonics generated looking into the spectrum of each signal
3. measure the rate of ODD and EVEN harmonics in the signals by dividing the quadratic sum of the first 10 harmonics by the amplitude of the fundamental frequency.
Feel free to comment ....
Following our previous topic here , this is a more complete and synthesized analysis (or an attempt to ) of the SOLDANO SLO 100-50 and 30 preamp . Remember that the point was to discover the part of that strange 3rd stage in the schematics of the OD channel here below :
The LTSpice simulation was therefore made from this schematic in which the red arrows show where the loaded output of the previous stage was measured :
The various computations made from the load lines and the correct formulas give this table :
Remember the low cut-off frequency due to the cathode RkCk network is given by :
The purpose is to characterize the sounds produced and more particularly the nature of the harmonics of the overtones resulting from overdriving the stages. We can make out the rate of ODD harmonics and EVEN harmonics.
So to start with we simulate with very common guitar PUs : the 490R and 498T Gibson humbuckers for which an approaching value of the ATTACK level can be found in the next table :
For example we see that the 498T outputs the maximum level with the 6th string at 1 Vpp , so the first stage with its 3 Vpp headroom will in no way be overdriven , which is a good thing since this stage is shared with the clean channel !
Now the complete channel is controlled with only one pot and it will be interesting to make it vary on the full range to see where we go : the lower values will be usefull to see what happens in the decreasing tails of the sustained overdriven notes.
Now the "log" pot . Of course with 11 graduations it is more precise than with 10 but for the computations it will be more simple to take 10 . Of course real logarithmic pots only exist in laboratories and not in our amps. What we call log pots are simply 2 linear pots in series , the second one having a far steeper slope than the first one . For each graduation the percentage of the input signal is this one :
So now I suggest we take a breath (
1. measure the various outputs of the stages with various inputs
2. identify for the various outputs the harmonics generated looking into the spectrum of each signal
3. measure the rate of ODD and EVEN harmonics in the signals by dividing the quadratic sum of the first 10 harmonics by the amplitude of the fundamental frequency.
Feel free to comment ....