You can see that only a portion of the middle signal is linear - output perfectly matches input. Now, don't panic because as circuit designers we have many ways to "linearize" this response curve which include different biasing schemes, feedback methods etc.
What's important to this discussion is that from a high-end perspective we would like a perfect device because the fewer tricks and schemes we employ to achieve a linear response from one extreme to another the better, cleaner and more open our musical presentation will be to a given piece of equipment.
There are no perfect devices - but remember in yesterday's post we mentioned that tubes run at much higher voltages than most transistors in a typical amplifying circuit? Think about the curve in the graph on this post which is showing the output voltage of a device. It should be obvious that the greater the voltage the greater the linear region.
Let's imagine that the graph represents 10 volts and the linear region is about 50%. That means that even on a good day you get a 5 volt linear region to play with - not a lot from a designer's standpoint. Now imagine that the same graph represented 100 volts which is a 10X increase - which gives us 50 volts of linear region! This is huge and more than we would ever need as designers.
From a sonic standpoint we hear image and apparent micro and macro compression as we get near the edges of our linear region and the ear picks these cues up immediately and recognizes something has changed. This is one of the primary reasons why most tube circuits sound so open, effortless and compression free at the quietest and the loudest extremes of the musical presentation. Think of this as a car analogy - if you have an oversized V8 engine in a small car, chances are good you won't notice any difference in performance from the slowest speeds to the fastest speeds. Change the engine out for a tiny 4-banger and your acceleration and top end speeds are compromised as the tiny engine struggles to do its best.
So while neither tubes nor transistors are true linear devices, the one with the highest voltage wins when it comes to an open and effortless soundstage with perfect micro and macro dynamics.
Notice that I didn't pick out tubes as the winner in this closing statement - just that used without a lot of knowledge to these effects, a pedestrian solid state audio designer (vs. a pedestrian tube audio designer) will always lose the sonic battle - hence, most tube designs sound more open and effortless than most solid state designs.
However, once armed with this knowledge we can have the freedom to express ourselves with either discipline - so as solid state designers we can choose our working voltages to take advantage of this knowledge. For example, in most every PS Audio amplification device we have always run two to three times the typical voltage used by other designers for this very reason. Others have done the same - but it is NOT common practice.
Tomorrow let's focus on one other difference between tubes and bipolar transistors, fields vs. solid connections.
High voltage and linearity
You can see that only a portion of the middle signal is linear - output perfectly matches input. Now, don't panic because as circuit designers we have many ways to "linearize" this response curve which include different biasing schemes, feedback methods etc.
What's important to this discussion is that from a high-end perspective we would like a perfect device because the fewer tricks and schemes we employ to achieve a linear response from one extreme to another the better, cleaner and more open our musical presentation will be to a given piece of equipment.
There are no perfect devices - but remember in yesterday's post we mentioned that tubes run at much higher voltages than most transistors in a typical amplifying circuit? Think about the curve in the graph on this post which is showing the output voltage of a device. It should be obvious that the greater the voltage the greater the linear region.
Let's imagine that the graph represents 10 volts and the linear region is about 50%. That means that even on a good day you get a 5 volt linear region to play with - not a lot from a designer's standpoint. Now imagine that the same graph represented 100 volts which is a 10X increase - which gives us 50 volts of linear region! This is huge and more than we would ever need as designers.
From a sonic standpoint we hear image and apparent micro and macro compression as we get near the edges of our linear region and the ear picks these cues up immediately and recognizes something has changed. This is one of the primary reasons why most tube circuits sound so open, effortless and compression free at the quietest and the loudest extremes of the musical presentation. Think of this as a car analogy - if you have an oversized V8 engine in a small car, chances are good you won't notice any difference in performance from the slowest speeds to the fastest speeds. Change the engine out for a tiny 4-banger and your acceleration and top end speeds are compromised as the tiny engine struggles to do its best.
So while neither tubes nor transistors are true linear devices, the one with the highest voltage wins when it comes to an open and effortless soundstage with perfect micro and macro dynamics.
Notice that I didn't pick out tubes as the winner in this closing statement - just that used without a lot of knowledge to these effects, a pedestrian solid state audio designer (vs. a pedestrian tube audio designer) will always lose the sonic battle - hence, most tube designs sound more open and effortless than most solid state designs.
However, once armed with this knowledge we can have the freedom to express ourselves with either discipline - so as solid state designers we can choose our working voltages to take advantage of this knowledge. For example, in most every PS Audio amplification device we have always run two to three times the typical voltage used by other designers for this very reason. Others have done the same - but it is NOT common practice.
Tomorrow let's focus on one other difference between tubes and bipolar transistors, fields vs. solid connections.
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