Constant current sources bleed in a constant current regardless of the voltage across them. So in this application, it feeds a constant current the source which is following the signal voltage, **regardless of ripple and trash on the negative supply**. The resistor will let the source current vary by I = V/R, and therefore mix in some of the trash and ripple which may exist on the negative supply.
In addition, a source- (or emitter-, or cathode-) follower has a gain nearer 1.000000 instead of nearly one as the equivalent resistance it sees as a load goes up. This is the "Rst" term in the equation I used. Constant current sources have equivalent resistances which are very, very high, so this pushes the follower to being a better, more ideal follower as well as reducing noise feedthrough.
Constant current sources were an expensive luxury back when you had to use an expensive tube to make them. But with $0.10 semiconductors, they are very, very nice additions.
In addition, a source- (or emitter-, or cathode-) follower has a gain nearer 1.000000 instead of nearly one as the equivalent resistance it sees as a load goes up. This is the "Rst" term in the equation I used. Constant current sources have equivalent resistances which are very, very high, so this pushes the follower to being a better, more ideal follower as well as reducing noise feedthrough.
Constant current sources were an expensive luxury back when you had to use an expensive tube to make them. But with $0.10 semiconductors, they are very, very nice additions.
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