The DC measured winding resistance is effectively in series with the AC reflected load. So your calculation of voltage "swing" would be correct. Just that it is AC swing, not DC swing. DC is non varying by definition. Only the V swing across the reflected AC load makes it to the load though (minus yet another secondary resistance component, and a small loss in the steel which shows up in the aprrox. 90 deg. magnetizing current for the core). So the +/- 20 mA AC component is said to be superimposed on the 50 mA DC component. Causing a 208 V P-P AC swing at the plate. Only 200 V P-P of which heads toward the load (minus another approx. 8 V P-P for the reflected equiv. secondary DC measured resistance loss).
It gets more complicated when you consider the distortion from the tube's non-linear gain. That +/- 20 mA component is more likely +22/-18 mA and the assymetry gets worse as the signal gets larger. This distortion caused shift is often referred to as a shift of the DC op. point (the 2 mA shift) if it is maintained by the larger signal envelope for some period of time. It really is an AC envelope (ie. lower frequency than the nominal signal) related shift. Frequencies lower than the nominal signal range are often referred to as DC shifts, conceptually helpful as long as everyone understands the intended meaning.
It gets more complicated when you consider the distortion from the tube's non-linear gain. That +/- 20 mA component is more likely +22/-18 mA and the assymetry gets worse as the signal gets larger. This distortion caused shift is often referred to as a shift of the DC op. point (the 2 mA shift) if it is maintained by the larger signal envelope for some period of time. It really is an AC envelope (ie. lower frequency than the nominal signal) related shift. Frequencies lower than the nominal signal range are often referred to as DC shifts, conceptually helpful as long as everyone understands the intended meaning.
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