I still believe you want to put that nominal 8 ohm load on the 4 ohm tap. ...
That reflects a double-normal primary impedance. I bet Ed knows the primary is 9.2kΩ by either measurement or asking MM. 8Ω of speaker on the 4Ω tap makes the primary impedance 18.4kΩ.
"Normal" for a SE EL34 would be in the range of 3-5kΩ for a single tube. So my suggestion of 8Ω on the 16Ω tap still only provides a good load for 1x EL34; 2x EL34 would be more-properly loaded by 2-3kΩ.
... Lets look at power draw, given the 1:1.4:2 voltage ratio typical of a 4-8-16 ohm output. Since power = volts*volts/resistance, you would have
1 squared over 8 or 1/8, versus 2 squared over 8, or 1/2. ...
The problem is the voltage ratios only hold if the same power is put through the OT in all settings. That is, if there is 15w of power output through the OT, the ratios of voltage between the taps is 1:1.4:2 but only if a 4Ω load is on the 4Ω tap, or an 8Ω load on the 8Ω tap, etc...
When you change the loading/mismatch, you change how the load impedance seen by the output tube, which changes its power output
before you consider the effect of differing voltage at different taps.
There is also a potential danger in an extremely high load impedance presented to an output tube driven hard: it makes the loadline cut way below the knee of the plate curves when pushed, and screen current can be excessive. It's enough of a problem that RCA's design procedure for output pentodes/beam power tubes was to draw multiple lines at different slopes radiating from the knee of the plate curves, and do the math to see which provides the best power output vs distortion.
... I agree with PRR that the power draw goes up as we crank up the gain (volume) ...
Power drawn
from the power supply stays the same from idle to full-roar because SE mandates class A operation. There will be a little bit of rise in current at full power, but that is due to distortion and rectification effects (in the output tube).
What actually happens is the tube dissipates the most power when it sits idle, but dissipates much less at full power output, because of the power transferred through the OT to the speaker.