Dertonarm, the use of the word 'feedback' in your posts above either has a new meaning for the term or else the term is misapplied (language issue). My theory is the latter right now.
There is an ideal loading for any inductive audio device wherein the device does not exhibit either ringing/overshoot (under-damped) or excessive rounding (overdamped).
This can be accomplished with or without a stepup transformer.
Loading can be used as a sort of tone control but is ill-advised, but sometimes very difficult to set up otherwise if the right equipment is not available (which is a 'scope and a squarewave generator). With the test equipment, the inductive device (cartridge) can be 'rung' by the square wave and the resulting waveform displayed on the scope. Without loading ringing will be observed. A load in parallel with the output of the device will cause the ringing to decrease- there will be some point where the ringing will cease altogether.
If loaded excessively, the corners of the square wave will be rounded. The debate about where critical damping lies centers around whether or not any overshoot is allowed (I tend to go for a slight amount). At this point the loading value will be only slightly higher- often the difference of only a few ohms.
A transformer can complicate the matter as the transformer can ring also. In addition, the load on the secondary will be 'transformed' by the transformer to a load on the cartridge, so if you are loading the secondary this must be taken into account. Jensen transformers has published a chart of how this is done with their transformers (they make some excellent SUTs BTW).
http://www.jensen-transformers.com/design/MC_Table.zip
There is an ideal loading for any inductive audio device wherein the device does not exhibit either ringing/overshoot (under-damped) or excessive rounding (overdamped).
This can be accomplished with or without a stepup transformer.
Loading can be used as a sort of tone control but is ill-advised, but sometimes very difficult to set up otherwise if the right equipment is not available (which is a 'scope and a squarewave generator). With the test equipment, the inductive device (cartridge) can be 'rung' by the square wave and the resulting waveform displayed on the scope. Without loading ringing will be observed. A load in parallel with the output of the device will cause the ringing to decrease- there will be some point where the ringing will cease altogether.
If loaded excessively, the corners of the square wave will be rounded. The debate about where critical damping lies centers around whether or not any overshoot is allowed (I tend to go for a slight amount). At this point the loading value will be only slightly higher- often the difference of only a few ohms.
A transformer can complicate the matter as the transformer can ring also. In addition, the load on the secondary will be 'transformed' by the transformer to a load on the cartridge, so if you are loading the secondary this must be taken into account. Jensen transformers has published a chart of how this is done with their transformers (they make some excellent SUTs BTW).
http://www.jensen-transformers.com/design/MC_Table.zip